JPH0453840B2 - - Google Patents

Info

Publication number
JPH0453840B2
JPH0453840B2 JP58060757A JP6075783A JPH0453840B2 JP H0453840 B2 JPH0453840 B2 JP H0453840B2 JP 58060757 A JP58060757 A JP 58060757A JP 6075783 A JP6075783 A JP 6075783A JP H0453840 B2 JPH0453840 B2 JP H0453840B2
Authority
JP
Japan
Prior art keywords
ingot
annealing
semiconductor manufacturing
temperature
semiconductor
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
Application number
JP58060757A
Other languages
Japanese (ja)
Other versions
JPS59190300A (en
Inventor
Hirobumi Shimizu
Masato Fujita
Kazuya Suzuki
Fumiaki Hanagata
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP58060757A priority Critical patent/JPS59190300A/en
Priority to FR8401838A priority patent/FR2543980A1/en
Priority to GB08404092A priority patent/GB2137524A/en
Priority to KR1019840001721A priority patent/KR840008533A/en
Priority to IT20408/84A priority patent/IT1175968B/en
Priority to DE19843413082 priority patent/DE3413082A1/en
Priority to FR8408514A priority patent/FR2543981A1/en
Publication of JPS59190300A publication Critical patent/JPS59190300A/en
Publication of JPH0453840B2 publication Critical patent/JPH0453840B2/ja
Granted legal-status Critical Current

Links

Classifications

    • CCHEMISTRY; METALLURGY
    • C30CRYSTAL GROWTH
    • C30BSINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B29/00Single crystals or homogeneous polycrystalline material with defined structure characterised by the material or by their shape
    • C30B29/02Elements
    • C30B29/06Silicon
    • 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
    • H10P95/00Generic processes or apparatus for manufacture or treatments not covered by the other groups of this subclass
    • CCHEMISTRY; METALLURGY
    • C30CRYSTAL GROWTH
    • C30BSINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B15/00Single-crystal growth by pulling from a melt, e.g. Czochralski method
    • C30B15/14Heating of the melt or the crystallised materials
    • CCHEMISTRY; METALLURGY
    • C30CRYSTAL GROWTH
    • C30BSINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B33/00After-treatment of single crystals or homogeneous polycrystalline material with defined structure

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  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Materials Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Crystals, And After-Treatments Of Crystals (AREA)

Description

【発明の詳細な説明】 [技術分野] 本発明は半導体製造技術、特に微小欠陥の少な
い半導体材料を得ることのできる半導体製造技術
に関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field] The present invention relates to a semiconductor manufacturing technology, and particularly to a semiconductor manufacturing technology that can obtain a semiconductor material with few micro defects.

[背景技術] 一般に、たとえばシリコン(Si)の結晶製造の
如き半導体製造過程においては、酸素ドナー解消
のためのインゴツトアニール(600〜650℃)が行
われることがある。一般には、φ100mm結晶以下
は第1図に示すようなインゴツトアニール法が、
φ125mm以上の結晶では第2図に示すようなウエ
ハアニール法が採用されている。
[Background Art] Generally, in a semiconductor manufacturing process such as silicon (Si) crystal manufacturing, ingot annealing (600 to 650° C.) is sometimes performed to eliminate oxygen donors. Generally, for crystals with a diameter of 100 mm or less, the ingot annealing method as shown in Figure 1 is used.
For crystals with a diameter of 125 mm or more, the wafer annealing method shown in Figure 2 is used.

単結晶インゴツトの直径が大きくなると、熱容
量が大きくなり急冷によつてクラツクが生じ易
く、現在φ125mm以上の結晶のアニールはウエハ
状態で行われている。このアニールは酸素ドナー
を消去し、インゴツトの長さ方向ならびに断面内
の抵抗率のばらつきを低減することを目的として
おり、微小欠陥の成長については核形成を促進す
る方向にある。
As the diameter of a single crystal ingot increases, its heat capacity increases and cracks are more likely to occur due to rapid cooling.Currently, crystals with a diameter of 125 mm or more are annealed in wafer form. The purpose of this annealing is to eliminate oxygen donors and reduce variations in resistivity in the longitudinal direction and cross section of the ingot, and to promote nucleation of microdefects.

ところで、現在使用されている半導体デバイス
の主流材料はシリコン結晶であり、その育成法と
してはチヨクラルスキー法(CZ法、引上法)と
フローテイングゾーン法(FZ法、帯溶融精製法)
がある。現在LSIを中心とするシリコンデバイス
に使う大部分のウエハはCZ法によつて育成して
いる。
By the way, the mainstream material for semiconductor devices currently in use is silicon crystal, and its growing methods include the Czyochralski method (CZ method, pulling method) and the floating zone method (FZ method, zone melting refining method).
There is. Currently, most wafers used for silicon devices, mainly LSI, are grown using the CZ method.

CZ法は、石英るつぼ内で多結晶シリコンを溶
融し、メルトに浸した種結晶とるつぼを相対的に
回転させながら種結晶を引き上げて結晶を育成す
る。CZ法で育成される結晶では、育成中の固液
界面での温度のゆらぎあるいは成長後の炉内熱輻
射の違いによつて単結晶インゴツトの各部分で微
小欠陥(酸素の析出)の核形成が変わつてくる。
In the CZ method, polycrystalline silicon is melted in a quartz crucible, and the seed crystal immersed in the melt is rotated relative to the crucible while the seed crystal is pulled up to grow a crystal. In crystals grown by the CZ method, micro defects (precipitation of oxygen) are nucleated in each part of the single crystal ingot due to temperature fluctuations at the solid-liquid interface during growth or differences in heat radiation in the furnace after growth. is changing.

また、核形成素度は酸素濃度の違いによつても
差が生ずる。
Further, the nucleation degree also varies depending on the oxygen concentration.

したがつて、一つのインゴツトからスライスし
て作られるウエハのバルク品質にはばらつきの要
素がある。たとえば、酸素が析出し易い結晶では
微小欠陥密度が高い。微小欠陥は転位発生中心と
なるので、スリツプの発生する臨界応力が低下す
る。したがつて、微小欠陥密度の高いウエハ程
LSIプロセスでの熱処理のさいスリツプやそりが
発生し易く、フオトリソグラフイ工程でのマスク
の転写精度を低下せしめる。一方、導入された熱
応力転位はデバイス特性を劣化し、歩留り低下の
原因となつている。
Therefore, there is an element of variation in the bulk quality of wafers sliced from a single ingot. For example, a crystal in which oxygen easily precipitates has a high microdefect density. Since micro defects serve as centers for dislocation generation, the critical stress at which slips occur is reduced. Therefore, the wafer with higher microdefect density
Slips and warpage are likely to occur during heat treatment in the LSI process, reducing mask transfer accuracy in the photolithography process. On the other hand, the introduced thermal stress dislocations deteriorate device characteristics and cause a decrease in yield.

近年、デバイスの高集積化、高性能化が著しく
進展し、微小欠陥に起因した結晶欠陥制御の問題
はプロセス面での最大感心事の一つになつてい
る。
In recent years, there has been significant progress in the integration and performance of devices, and the problem of crystal defect control caused by micro defects has become one of the biggest concerns in terms of process.

固体撮像素子では結晶欠陥の存在が画像に白点
不良をもたらし、歩留り低下の最大の原因となつ
ている。
In solid-state imaging devices, the presence of crystal defects causes white spot defects in images, which is the biggest cause of yield decline.

第3図はCMOS5μmプロセスで実装して得ら
れたφ100ウエハのそりと微小欠陥密度の関係で
ある。微小欠陥密度が高い程そり量が大きくなつ
ていることがわかる。第3図はN2アニール工程
完で抜き取つたウエハのそりを測定している。
Figure 3 shows the relationship between warpage and microdefect density of a φ100 wafer mounted using a CMOS 5μm process. It can be seen that the higher the microdefect density, the greater the amount of warpage. Figure 3 measures the warpage of a wafer extracted after completing the N2 annealing process.

微小欠陥密度は1000℃で16時間酸化後、40μm
深さで測定した値である。
Micro defect density is 40μm after oxidation at 1000℃ for 16 hours
This is a value measured in depth.

参考のため強制熱処理シミユレーシヨンで得た
そりと微小欠陥密度の相関を実験結果として第4
図と第5図に示す。
For reference, the correlation between warpage and microdefect density obtained through forced heat treatment simulation is shown in the fourth section as an experimental result.
As shown in Fig. and Fig. 5.

このそり評価実験は2段の強制熱処理を行うも
ので、このそり評価に用いた熱処理炉の石英管の
内径は150mmであり、2段の強制熱処理()、
()は次の条件で行われた。
This warpage evaluation experiment performed two-stage forced heat treatment. The inner diameter of the quartz tube of the heat treatment furnace used for this warpage evaluation was 150 mm, and two-stage forced heat treatment (),
() was conducted under the following conditions.

強制熱処理 () 1000℃、20min(保持) ウエハ間隔:5mm 出入れ速度:20cm/min 強制熱処理 () 1000℃、20min(保持) ウエハ間隔:5mm 出入れ速度:35cm/min なお、この実験では各熱処理のそり量からウエ
ハの初期そりを差し引いているので、そりは強制
熱処理で組成変形した正味の値を示している。
Forced heat treatment () 1000℃, 20min (holding) Wafer spacing: 5mm Input/output speed: 20cm/min Forced heat treatment () 1000℃, 20min (holding) Wafer spacing: 5mm Input/output speed: 35cm/min Note that in this experiment, each Since the initial warpage of the wafer is subtracted from the amount of warpage due to heat treatment, the warpage represents the net value of compositional deformation due to forced heat treatment.

800℃−1000℃の2段熱処理を行えば、微小欠
陥密度が高くなり、そり易くなる。
If two-stage heat treatment is performed at 800°C-1000°C, the density of minute defects will increase, making it easier to warp.

第4図と第5図の破線は育成条件の異なるイン
ゴツトから採取した比較ウエハで得た結果であ
る。
The broken lines in FIGS. 4 and 5 represent the results obtained with comparison wafers taken from ingots grown under different growth conditions.

これらの結果は、たとえば結晶中の酸素濃度の
値が変われば、微小欠陥の核形成、成長が異な
り、スリツプの発生し易さが違うことを示してい
る。
These results show that, for example, if the oxygen concentration in the crystal changes, the nucleation and growth of micro defects will differ, and the ease with which slips will occur will differ.

このように、熱応力によるそりは単結晶の品
質、特に酸素の析出状態(微小欠陥密度)に強く
依存する。
As described above, warping due to thermal stress strongly depends on the quality of the single crystal, especially on the state of oxygen precipitation (microdefect density).

第3図でそりが〜70μmを越せばCMOSの5μm
プロセスでもフオトエツチング工程での転写精度
が悪くなり、素子歩留りが悪化することが知られ
ている。今後、高集積化が進むにつれて、それを
もつと小さくする必要が生じている。
In Figure 3, if the warpage exceeds ~70μm, the CMOS will be 5μm.
It is also known that the transfer accuracy in the photoetching process deteriorates, and the device yield deteriorates. In the future, as higher integration progresses, there will be a need to make them smaller.

このような要求を満足させるため素子プロセス
面では熱処理のさい炉熱炉冷(Ramping)が徹
底されつつある。一方、800〜900℃から
Rampingを行えば酸素析出の核が生じ易く、微
小欠陥が成長し易くなるため結晶の強度は低下す
る。したがつて、熱処理にも酸素が析出しにく
い、すなわち微小欠陥の核の少ない、均質な結晶
に対する要求が強くなつている。
In order to satisfy these demands, in the device process, furnace cooling (ramping) is becoming more and more popular during heat treatment. Meanwhile, from 800-900℃
If ramping is performed, oxygen precipitation nuclei are likely to occur, and micro defects are likely to grow, resulting in a decrease in the strength of the crystal. Therefore, there is an increasing demand for homogeneous crystals that are less likely to cause oxygen to precipitate during heat treatment, that is, have fewer microdefect nuclei.

[発明の目的] 本発明の目的は、半導体材料における微小欠陥
の核を減少させることのできる半導体製造技術を
提供することにある。
[Object of the Invention] An object of the present invention is to provide a semiconductor manufacturing technique that can reduce the number of microdefect nuclei in a semiconductor material.

本発明の他の目的は、半導体材料の結晶にクラ
ツクが発生することを防止できる半導体製造技術
を提供することにある。
Another object of the present invention is to provide a semiconductor manufacturing technique that can prevent cracks from occurring in the crystal of a semiconductor material.

本発明の前記ならびにその他の目的と新規な特
徴は、本明細書の記述および添付図面から明らか
になるであろう。
The above and other objects and novel features of the present invention will become apparent from the description of this specification and the accompanying drawings.

[発明の概要] 本願において開示される発明のうち代表的なも
のの概要を簡単に説明すれば、次の通りである。
[Summary of the Invention] A brief overview of typical inventions disclosed in this application is as follows.

すなわち、半導体材料のインゴツトを輻射熱で
加熱した後、所定温度まで急冷し、その所定温度
に所定時間保持することにより、微小欠陥の核
(酸素析出の核)の形成を防止し、またインゴツ
トにクラツクが発生することを防止することがで
きる。
That is, by heating an ingot of a semiconductor material with radiant heat, rapidly cooling it to a predetermined temperature, and holding it at that predetermined temperature for a predetermined period of time, it is possible to prevent the formation of microdefect nuclei (nuclei of oxygen precipitation) and to prevent cracks in the ingot. can be prevented from occurring.

[実施例] 第6図は本発明による半導体製造装置の一実施
例を示す概略断面図である。
[Embodiment] FIG. 6 is a schematic cross-sectional view showing an embodiment of a semiconductor manufacturing apparatus according to the present invention.

本実施例においては、アニール用の熱処理炉は
透明な石英ベルジヤー1で構成された縦型炉構造
であり、石英ベルジヤー1の頂部には蓋2が設け
られている。
In this embodiment, the annealing heat treatment furnace has a vertical furnace structure composed of a transparent quartz bell jar 1, and a lid 2 is provided on the top of the quartz bell jar 1.

この石英ベルジヤー1の中には、ガス導入口3
から非酸化性の雰囲気ガス4、たとえば窒素また
はアルゴンガス等の不活性ガスが供給されてい
る。
Inside this quartz bell gear 1, there is a gas inlet 3.
A non-oxidizing atmospheric gas 4, for example an inert gas such as nitrogen or argon gas, is supplied from the tank.

一方、前記石英ベルジヤー1の内部には、たと
えばシリコンの単結晶よりなるインゴツト5が装
入され、このインゴツト5は石英ベルジヤー1の
上方においてチヤツク7で固定され、0〜30r.p.
m.の速度で回転可能に支持されている。本実施
例のインゴツト5は上部に種結晶5aが残された
ままであり、種結晶5aは育成されたインゴツト
5から切り離されておらず、本実施例の1つの特
徴となつている。
On the other hand, an ingot 5 made of, for example, a single crystal of silicon is charged inside the quartz bell gear 1, and this ingot 5 is fixed with a chuck 7 above the quartz bell gear 1, and is heated at 0 to 30 r.p.
supported for rotation at a speed of m. The seed crystal 5a remains in the upper part of the ingot 5 of this embodiment, and the seed crystal 5a is not separated from the grown ingot 5, which is one of the features of this embodiment.

また、本実施例の装置では、アニール用の加熱
源として輻射熱源が使用されており、この輻射熱
源は赤外線ランプ6よりなる。赤外線ランプ6は
石英ベルジヤー1の外周側に配置されており、そ
の電源をON、OFFさせることによつてインゴツ
ト5を非接触で加熱してアニールし、また急冷す
ることができる。
Further, in the apparatus of this embodiment, a radiant heat source is used as a heat source for annealing, and this radiant heat source is composed of an infrared lamp 6. The infrared lamp 6 is arranged on the outer peripheral side of the quartz bell gear 1, and by turning the power on and off, the ingot 5 can be heated and annealed without contact, and can be rapidly cooled.

次に、本実施例によりシリコンの単結晶のイン
ゴツトをアニールする場合の作用について説明す
る。
Next, the operation when a silicon single crystal ingot is annealed according to this embodiment will be explained.

まず、第6図に示すように石英ベルジヤー1内
に非接触状態で支持したインゴツト5を図示しな
い回転手段で回転させながら、赤外線ランプ6か
らの赤外線6aによりインゴツト5をたとえば
1200〜1350℃に加熱し、数時間保持し、アニール
する。アニール効果を上げるためには加熱温度は
高い方が望ましい。
First, as shown in FIG. 6, while the ingot 5 supported in a non-contact manner in the quartz bell jar 1 is rotated by a rotating means (not shown), the ingot 5 is heated by infrared rays 6a from an infrared lamp 6, for example.
Heat to 1200-1350℃ and hold for several hours to anneal. In order to improve the annealing effect, it is desirable that the heating temperature be higher.

第7図には、1200℃と1350℃の2つのアニール
温度でアニールする場合の例を示している。
FIG. 7 shows an example of annealing at two annealing temperatures of 1200°C and 1350°C.

これらのアニール温度で所定時間のアニールを
行つた後、赤外線ランプ6の出力を落とし、急冷
する。この急冷の際の温度プログラムは第7図に
示されている。
After performing annealing for a predetermined time at these annealing temperatures, the output of the infrared lamp 6 is reduced to rapidly cool. The temperature program during this rapid cooling is shown in FIG.

第7図の温度プログラムでは、まず最初には10
〜15℃/minの冷却速度で冷却し、次に約1100℃
から300℃まで25〜100℃/minの冷却速度で急冷
することにより二段階の冷却速度での急冷が行わ
れる。
The temperature program in Figure 7 starts with 10
Cool at a cooling rate of ~15°C/min, then approximately 1100°C
By rapidly cooling from 300°C to 300°C at a cooling rate of 25 to 100°C/min, rapid cooling is performed at two stages of cooling rates.

この急冷操作において、1100℃〜650℃ではイ
ンゴツト5における微小欠陥の核の再形成を抑制
し、650℃〜400℃では酸素ドナーの再形成を抑制
するという作用効果が得られる。
In this rapid cooling operation, the effects of suppressing the re-formation of nuclei of micro defects in the ingot 5 at 1100°C to 650°C and suppressing the re-formation of oxygen donors at 650°C to 400°C are obtained.

また、300℃で一時保持しているのは、急冷の
際に生じる熱歪でインゴツト5にクラツクが発生
するのを防止するためである。
Further, the reason why the temperature is temporarily maintained at 300°C is to prevent cracks from occurring in the ingot 5 due to thermal distortion caused during rapid cooling.

なお、300℃以下は所定時間後にさらに急冷を
行うことができ、その場合の冷却速度は前記した
2段階の急冷時とは異なる冷却速度にすることが
できる。
Note that when the temperature is 300° C. or lower, further rapid cooling can be performed after a predetermined period of time, and the cooling rate in this case can be set to a different cooling rate from the two-stage rapid cooling described above.

本実施例によれば、非接触状態でシリコン単結
晶インゴツト5を高温アニールできるので、汚染
を心配することなく単結晶育成中および炉内熱履
歴によつて作られた微小欠陥の核(酸素析出の
核)を固溶せしめることができる。また、赤外線
ランプ6による輻射加熱方式のため通常の抵抗加
熱式に比較して結晶を急冷することが可能であ
る。
According to this embodiment, since the silicon single crystal ingot 5 can be annealed at high temperature in a non-contact state, the nuclei of minute defects (oxygen precipitation, ) can be dissolved in solid solution. In addition, since it uses a radiation heating method using an infrared lamp 6, it is possible to cool the crystal more rapidly than in a normal resistance heating method.

したがつて、冷却中過飽和な酸素が集合し微小
欠陥の核となる過程を抑制できる。このような単
結晶インゴツト5からスライスしてミラー加工し
たシリコンウエハは、LSIのプロセスでも酸素の
析出が起こりにくく、したがつて微小な転位ルー
プや、酸化誘起積層欠陥の発生が極めて少ない。
Therefore, it is possible to suppress the process in which supersaturated oxygen aggregates during cooling and becomes the nucleus of micro defects. A silicon wafer sliced from such a single crystal ingot 5 and subjected to mirror processing is less prone to oxygen precipitation even in the LSI process, and therefore has extremely few occurrences of minute dislocation loops and oxidation-induced stacking faults.

現在、単結晶評価法としてバルク内の微小欠陥
密度を調べる方法が用いられている。この方法で
は、ウエハを1000℃で10数時間酸化し、表面を〜
40μm鏡面研磨した後、ライト(light)エツチ液
で5分間エツチングする。規定の場所の欠陥数を
求め体積密度(個/cm3)に換算する。
Currently, a method of examining the microdefect density in the bulk is used as a single crystal evaluation method. In this method, the wafer is oxidized at 1000℃ for 10 hours, and the surface is
After mirror polishing to 40 μm, etching was performed using light etchant for 5 minutes. The number of defects at a specified location is determined and converted to volumetric density (pieces/cm 3 ).

この方法によれば、一般の結晶のレベルは107
〜108個/cm3にあるのに対し、本実施例の方法
(ウエハアニールの実験結果)では105個/cm3以下
のレベルを実現している。LSIプロセスの低温化
が進められつつある現在、結晶はますます厳しい
条件で使われることになり、そのためには、本実
施例は極めて有用である。
According to this method, the level of general crystals is 10 7
In contrast, the method of this embodiment (experimental results of wafer annealing) achieves a level of 10 5 particles /cm 3 or less . Nowadays, as the temperature of LSI processes is being lowered, crystals are being used under increasingly severe conditions, and this embodiment is extremely useful for this purpose.

[効果] (1) 本発明によりアニールされたインゴツトには
微小欠陥の核(酸素析出の核)が非常に少な
く、良好な特製の半導体素子を歩留り良く得る
ことができる。
[Effects] (1) The ingot annealed according to the present invention has very few nuclei of micro defects (nuclei of oxygen precipitation), and it is possible to obtain good specially manufactured semiconductor devices with a high yield.

(2) インゴツトをアニール後に所定温度まで急冷
し、その所定温度に所定時間保持することによ
り、インゴツトのクラツクの発生を防止するこ
とができる。
(2) By rapidly cooling the ingot to a predetermined temperature after annealing and holding the ingot at that predetermined temperature for a predetermined period of time, it is possible to prevent the occurrence of cracks in the ingot.

以上本発明者によつてなされた発明を実施例に
もとづき具体的に説明したが、本発明は前記実施
例に限定されるものではなく、その要旨を逸脱し
ない範囲で種々変更可能であることはいうまでも
ない。
Although the invention made by the present inventor has been specifically explained above based on examples, the present invention is not limited to the above-mentioned examples, and it is understood that various changes can be made without departing from the gist of the invention. Needless to say.

たとえば、インゴツトの急冷の速度はアニール
温度や半導体材料の種類に応じて様々に変えるこ
とができる。
For example, the rate of quenching the ingot can be varied depending on the annealing temperature and the type of semiconductor material.

また、インゴツトに対してだけでなくスライス
したウエハに本発明の方法を適用できる。
Further, the method of the present invention can be applied not only to ingots but also to sliced wafers.

さらに、輻射熱源としても赤外線ランプ以外に
高周波コイル等を利用することもできる。
Furthermore, a high frequency coil or the like can also be used as a radiant heat source in addition to an infrared lamp.

[利用分野] 以上の説明では主として本発明者によつてなさ
れた発明をその背景となつた利用分野であるシリ
コン単結晶インゴツトのアニールに適用した場合
について説明したが、それに限定されるものでは
なく、たとえば、ガリウム−砒素(Ga−As)、
ガリウム−リン(Ga−P)等の−族化合物
半導体あるいは−族化合物半導体等にも適用
できる。その場合のアニール温度はたとえば
0.85Tk〜0.95Tk(Tk:融点、ただし絶対温度表
示)にするのが望ましい。
[Field of Application] In the above explanation, the invention made by the present inventor was mainly applied to the application field of annealing of silicon single crystal ingots, which is the background of the invention, but the present invention is not limited thereto. , for example, gallium-arsenide (Ga-As),
It can also be applied to - group compound semiconductors such as gallium-phosphide (Ga-P) or - group compound semiconductors. For example, the annealing temperature in that case is
It is desirable to set the temperature to 0.85Tk to 0.95Tk (Tk: melting point, expressed as absolute temperature).

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

第1図はインゴツトアニール法の諸工程を示す
図、第2図はウエハアニール法の諸工程を示す
図、第3図はN2アニール後のウエハのそりと微
小欠陥密度との関係を示す図、第4図は強制熱処
理によるウエハのそりと微小欠陥密度の関係を示
す図、第5図も同様に別の強制熱処理によるウエ
ハのそりと微小欠陥密度との関係を示す図、第6
図は本発明による半導体製造装置の一実施例を示
す略断面図、第7図は本発明におけるアニールお
よび急冷の温度プログラムを示す図である。 1……石英ベルジヤー(炉)、2……蓋、3…
…ガス導入口、4……雰囲気ガス、5……インゴ
ツト、5a……種結晶、6……赤外線ランプ(輻
射熱源)、6a……赤外線、7……チヤツク。
Figure 1 shows the steps of the ingot annealing method, Figure 2 shows the steps of the wafer annealing method, and Figure 3 shows the relationship between wafer warpage and microdefect density after N 2 annealing. Figure 4 is a diagram showing the relationship between wafer warpage and microdefect density due to forced heat treatment, Figure 5 is a diagram showing the relationship between wafer warpage and microdefect density due to another forced heat treatment, and Figure 6
The figure is a schematic sectional view showing an embodiment of the semiconductor manufacturing apparatus according to the present invention, and FIG. 7 is a diagram showing a temperature program for annealing and rapid cooling in the present invention. 1...quartz bell jar (furnace), 2...lid, 3...
...Gas inlet, 4...Atmospheric gas, 5...Ingot, 5a...Seed crystal, 6...Infrared lamp (radiant heat source), 6a...Infrared rays, 7...Chick.

Claims (1)

【特許請求の範囲】 1 半導体材料を高温でアニールする半導体製造
方法において、半導体材料のインゴツトを輻射熱
で加熱してアニールした後、所定温度まで急冷
し、その所定温度に所定時間保持することを特徴
とする半導体製造方法。 2 急冷なインゴツトの温度に応じて複数段の異
なる冷却速度で行われることを特徴とする特許請
求の範囲第1項記載の半導体製造方法。 3 半導体材料を高温でアニールする半導体製造
装置において、半導体材料のインゴツトを炉内に
非接触状態で保持すると共に、インゴツトを輻射
状態で加熱する輻射熱源を設けたことを特徴とす
る半導体製造装置。 4 輻射熱源が赤外線ランプよりなることを特徴
とする特許請求の範囲第3項記載の半導体製造装
置。
[Claims] 1. A semiconductor manufacturing method in which a semiconductor material is annealed at a high temperature, characterized by heating an ingot of the semiconductor material with radiant heat to anneal it, then rapidly cooling it to a predetermined temperature, and holding the ingot at the predetermined temperature for a predetermined period of time. A semiconductor manufacturing method. 2. The semiconductor manufacturing method according to claim 1, wherein the cooling is performed at different cooling rates in multiple stages depending on the temperature of the rapidly cooled ingot. 3. A semiconductor manufacturing apparatus for annealing semiconductor materials at high temperatures, characterized in that an ingot of the semiconductor material is held in a furnace in a non-contact state, and a radiant heat source is provided for heating the ingot in a radiant state. 4. The semiconductor manufacturing apparatus according to claim 3, wherein the radiant heat source is an infrared lamp.
JP58060757A 1983-04-08 1983-04-08 Method and apparatus for production of semiconductor Granted JPS59190300A (en)

Priority Applications (7)

Application Number Priority Date Filing Date Title
JP58060757A JPS59190300A (en) 1983-04-08 1983-04-08 Method and apparatus for production of semiconductor
FR8401838A FR2543980A1 (en) 1983-04-08 1984-02-07 PROCESS FOR PRODUCING SEMICONDUCTOR MATERIALS AND PROCESSING FURNACE FOR CARRYING OUT SAID METHOD
GB08404092A GB2137524A (en) 1983-04-08 1984-02-16 A process for fabricating a semiconductor material and an apparatus therefor
KR1019840001721A KR840008533A (en) 1983-04-08 1984-04-02 Method for manufacturing semiconductor material and apparatus for use therein
IT20408/84A IT1175968B (en) 1983-04-08 1984-04-05 PROCEDURE FOR MANUFACTURING SEMICONDUCTOR MATERIALS AND RELATED EQUIPMENT
DE19843413082 DE3413082A1 (en) 1983-04-08 1984-04-06 METHOD AND DEVICE FOR PRODUCING SEMICONDUCTOR MATERIALS
FR8408514A FR2543981A1 (en) 1983-04-08 1984-05-30 PROCESS FOR PRODUCING SEMICONDUCTOR MATERIALS AND PROCESSING FURNACE FOR CARRYING OUT SAID METHOD

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58060757A JPS59190300A (en) 1983-04-08 1983-04-08 Method and apparatus for production of semiconductor

Publications (2)

Publication Number Publication Date
JPS59190300A JPS59190300A (en) 1984-10-29
JPH0453840B2 true JPH0453840B2 (en) 1992-08-27

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Application Number Title Priority Date Filing Date
JP58060757A Granted JPS59190300A (en) 1983-04-08 1983-04-08 Method and apparatus for production of semiconductor

Country Status (6)

Country Link
JP (1) JPS59190300A (en)
KR (1) KR840008533A (en)
DE (1) DE3413082A1 (en)
FR (2) FR2543980A1 (en)
GB (1) GB2137524A (en)
IT (1) IT1175968B (en)

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Also Published As

Publication number Publication date
IT8420408A0 (en) 1984-04-05
JPS59190300A (en) 1984-10-29
GB2137524A (en) 1984-10-10
FR2543980A1 (en) 1984-10-12
FR2543981A1 (en) 1984-10-12
DE3413082A1 (en) 1984-10-11
IT1175968B (en) 1987-08-12
GB8404092D0 (en) 1984-03-21
KR840008533A (en) 1984-12-15

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