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JP2621069B2 - Method for producing semiconductor silicon single crystal by FZ method - Google Patents
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JP2621069B2 - Method for producing semiconductor silicon single crystal by FZ method - Google Patents

Method for producing semiconductor silicon single crystal by FZ method

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Publication number
JP2621069B2
JP2621069B2 JP3201348A JP20134891A JP2621069B2 JP 2621069 B2 JP2621069 B2 JP 2621069B2 JP 3201348 A JP3201348 A JP 3201348A JP 20134891 A JP20134891 A JP 20134891A JP 2621069 B2 JP2621069 B2 JP 2621069B2
Authority
JP
Japan
Prior art keywords
single crystal
heating coil
coil
eccentricity
diameter
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
JP3201348A
Other languages
Japanese (ja)
Other versions
JPH0524966A (en
Inventor
泰弘 池田
勝己 市村
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.)
Shin Etsu Handotai Co Ltd
Original Assignee
Shin Etsu Handotai Co Ltd
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Filing date
Publication date
Application filed by Shin Etsu Handotai Co Ltd filed Critical Shin Etsu Handotai Co Ltd
Priority to JP3201348A priority Critical patent/JP2621069B2/en
Publication of JPH0524966A publication Critical patent/JPH0524966A/en
Application granted granted Critical
Publication of JP2621069B2 publication Critical patent/JP2621069B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Crystals, And After-Treatments Of Crystals (AREA)

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は原料多結晶を高周波誘導
加熱コイルを用いて、部分的に加熱溶融しその溶融帯域
を移動させることによって、単結晶成長を行うFZ法半
導体単結晶の製造に於いて、特に単結晶棒の断面内に均
一な電気抵抗率を持つシリコン単結晶棒の製造方法に関
する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for producing a single crystal of an FZ method in which a raw material polycrystal is partially heated and melted by using a high-frequency induction heating coil and the melting zone is moved to grow a single crystal. In particular, the present invention relates to a method for manufacturing a silicon single crystal rod having a uniform electric resistivity in a cross section of the single crystal rod.

【0002】[0002]

【従来の技術】従来、上軸に棒状原料多結晶を、下軸に
直径の小さい単結晶の種を保持し、高周波誘導加熱コイ
ルにより多結晶の一端を溶融し、前記種結晶に融着して
種付けした後、種絞りにより無転位化しつつ多結晶を反
対方向に回転させ、かつ軸線方向に相対移動させつつ前
記半導体棒を帯域溶融させながら棒状半導体単結晶を製
造する装置はFZ法半導体単結晶製造装置として知られ
ている。
2. Description of the Related Art Conventionally, a rod-shaped raw material polycrystal is held on an upper axis, and a single crystal seed having a small diameter is held on a lower axis. One end of the polycrystal is melted by a high frequency induction heating coil and fused to the seed crystal. After the seeding, the apparatus for producing a rod-shaped semiconductor single crystal while zone melting the semiconductor rod while rotating the polycrystal in the opposite direction while dislocation-free by the seed drawing and relatively moving in the axial direction is an FZ method semiconductor single. Known as a crystal manufacturing apparatus.

【0003】この装置においては、原料多結晶を狭小域
に於いて短時間に芯まで溶融させる必要から、半導体棒
の帯域溶融域に集中して電界を付加し得ることが必要で
あり、一方帯域溶融後の半導体を不純物のバラツキ等が
無く、かつ熱歪みを抑制し安定して単結晶を成長させる
には前記浮遊帯域と接する単結晶成長界面の成長開始端
側を緩かに放熱させる必要がある。
In this apparatus, since it is necessary to melt the raw material polycrystal to the core in a short time in a narrow area, it is necessary to be able to apply an electric field concentrated on the zone melting area of the semiconductor rod. In order to stably grow a single crystal without a variation in impurities in the semiconductor after melting, and to suppress thermal distortion, it is necessary to gently radiate heat at the growth start end side of the single crystal growth interface in contact with the floating zone. is there.

【0004】更に上記の不純物のバラツキ等を無くし、
断面内の電気抵抗率を均一にするため、溶融帯域中の攪
拌を効率的に行うのが良いとされ、成長中のシリコン単
結晶を高速に回転させて強制攪拌することも考えられる
が、溶融帯域が遠心力で外周部に移動したり前記単結晶
棒下方先端に成形した絞り部で結晶棒の重量を支えてい
るため、高速回転には耐えられず、成長中の単結晶棒が
倒壊してしまう等の不都合な現象がおきるのでこの手段
はとれない。
[0004] Further, the above-mentioned dispersion of impurities is eliminated,
It is considered good to efficiently stir the melting zone in order to make the electrical resistivity in the cross section uniform, and it is conceivable to rotate the growing silicon single crystal at high speed and forcibly stir. Since the zone moves to the outer peripheral part by centrifugal force or supports the weight of the crystal rod by the narrowed part formed at the lower end of the single crystal rod, it cannot withstand high-speed rotation, and the growing single crystal rod collapses. This measure cannot be taken because of inconvenient phenomena such as inconvenience.

【0005】このような従来技術の問題点を一挙に解決
すべく、本発明者は多結晶外径より小なる内径を有する
第一の単巻誘導加熱コイルと、前記第一のコイル内径よ
り大なる内径を有し、少なくともその内縁側を単結晶成
長界面の成長開始端側周縁部に対峙せしめた第二の誘導
加熱コイルとを含み、前記第一のコイルにより原料多結
晶の帯域溶融を行いつつ、第二のコイルにより単結晶成
長開始端側周縁部を加熱しながらその放熱速度を制御可
能に構成しつつ、帯域溶融と単結晶の成長を効率良くか
つ不純物分布のバラツキを低減しつつ容易に大口径かつ
高品質の単結晶を製造するようにしたFZ法半導体単結
晶製造装置を既に提案した。(特開昭63ー29188
7号公報)
In order to alleviate the problems of the prior art, the inventor of the present invention has proposed a first single-turn induction heating coil having an inner diameter smaller than the outer diameter of a polycrystal and a first coil having a larger inner diameter than the first coil. A second induction heating coil having an inner diameter of at least the inner edge side of which faces the growth start end side peripheral portion of the single crystal growth interface, and performs zone melting of the raw material polycrystal by the first coil. In addition, the second coil heats the peripheral edge of the single crystal growth starting end while controlling the heat release rate, and facilitates zone melting and single crystal growth efficiently while reducing variation in impurity distribution. Has already proposed an FZ method semiconductor single crystal manufacturing apparatus capable of manufacturing a large-diameter and high-quality single crystal. (JP-A-63-29188)
No. 7)

【0006】[0006]

【発明が解決しようとする課題】本発明は、前記FZ法
半導体単結晶製造装置をもちいて製品の単結晶棒断面内
の電気抵抗分布のバラツキを低減することができるFZ
法による半導体シリコン単結晶の製造方法を提供するこ
とを目的とする。
SUMMARY OF THE INVENTION According to the present invention, there is provided an FZ method capable of reducing a variation in electric resistance distribution in a cross section of a single crystal rod of a product by using the FZ method semiconductor single crystal manufacturing apparatus.
It is an object of the present invention to provide a method for manufacturing a semiconductor silicon single crystal by a method.

【0007】[0007]

【課題を解決するための手段】上記課題を解決するため
に、本発明のFZ法による半導体シリコン単結晶の製造
方法は、内側に位置する第一加熱コイルと、外側に位置
する第二加熱コイルを設置し該第一加熱コイルの中心軸
と原料多結晶の中心軸とを同軸にし、かつ該第二加熱コ
イルの中心軸と単結晶の中心軸とを同軸に配置し、かつ
単結晶の口径によって単結晶の回転数及び、第一加熱コ
イルと第二加熱コイルの偏芯量を選択するようにしたも
のである。
In order to solve the above-mentioned problems, a method for producing a semiconductor silicon single crystal by the FZ method according to the present invention comprises a first heating coil located inside and a second heating coil located outside. And the central axis of the first heating coil and the central axis of the raw material polycrystal are coaxial, and the central axis of the second heating coil and the central axis of the single crystal are arranged coaxially, and the diameter of the single crystal Thus, the rotation speed of the single crystal and the eccentricity of the first heating coil and the second heating coil are selected.

【0008】即ち、前記FZ法半導体単結晶製造装置に
おいて、単結晶棒の断面内の電気抵抗率分布のバラツキ
を低減するために、更に詳細に単結晶製造条件を追求し
た結果、好ましくは内側に位置する第一加熱コイルと外
側に位置する第二加熱コイルを互いに偏芯して設け、更
に第一加熱コイルの中心軸と原料多結晶の中心軸を同軸
に配置し、かつ前記第二コイルの中心軸と単結晶の中心
軸とを同軸に配置するのがよいことを見出したものであ
る。
That is, in the FZ method semiconductor single crystal manufacturing apparatus, as a result of pursuing the single crystal manufacturing conditions in more detail in order to reduce the variation of the electric resistivity distribution in the cross section of the single crystal rod, it is preferable that The first heating coil located and the second heating coil located outside are provided eccentrically to each other, and furthermore, the central axis of the first heating coil and the central axis of the raw material polycrystal are arranged coaxially, and It has been found that it is better to arrange the central axis and the central axis of the single crystal coaxially.

【0009】更に単結晶の口径によって、単結晶棒の回
転数と第一、第二加熱コイルの偏芯量を調節することが
目的を達成するに有利であることを提案するものであ
る。
Further, it is proposed that adjusting the rotation speed of the single crystal rod and the amount of eccentricity of the first and second heating coils according to the diameter of the single crystal is advantageous for achieving the object.

【0010】この際、単結晶の口径が約2.5”の場合
には、単結晶回転数8〜30回/分に対し偏芯量が6〜
12ミリメートル、単結晶の口径が約4.0”の場合に
は、単結晶回転数3〜12回/分に対し偏芯量4〜14
ミリメートル、又単結晶口径が約5”の場合には、単結
晶回転数2〜6回/分に対し偏芯量3〜16ミリメート
ルの時、単結晶棒断面内の電気抵抗が最も均一になる。
At this time, when the diameter of the single crystal is about 2.5 ", the eccentricity is 6 to 10 with respect to the rotation speed of the single crystal of 8 to 30 times / min.
When the diameter of the single crystal is 12 mm and the diameter of the single crystal is about 4.0 ″, the eccentricity is 4 to 14 with respect to the rotation speed of the single crystal 3 to 12 times / min.
When the diameter of the single crystal is about 5 "and the eccentricity is 3 to 16 mm with respect to the rotation rate of the single crystal of 2 to 6 times / minute, the electric resistance in the cross section of the single crystal rod becomes the most uniform. .

【0011】[0011]

【作用】特開昭63−291887号公報明細書及び図
面に開示するFZ法半導体単結晶製造装置は、第1コイ
ルは原料多結晶の浮遊帯域溶融を行ない、他方第2コイ
ルは単結晶成長開始端周縁部にその内径円周端を対峙さ
せることによってゆるやかに加熱し、単結晶成長界面芯
部分と外側部分との温度差を極力抑制することによって
単結晶成長界面の湾曲程度が浅くなり、単結晶棒断面内
の不純物分布、即ち電気抵抗率分布のバラツキが低減さ
れるという効果を奏するものである。
In the FZ method semiconductor single crystal manufacturing apparatus disclosed in Japanese Patent Application Laid-Open No. 63-291887 and drawings, the first coil melts the floating zone of the raw material polycrystal, while the second coil starts the single crystal growth. The inner peripheral edge of the single crystal growth interface is gently heated by confronting the inner peripheral edge with the peripheral edge, and the temperature difference between the single crystal growth interface core portion and the outer portion is suppressed as much as possible. This has the effect of reducing the variation in the impurity distribution in the crystal rod cross section, that is, the variation in the electrical resistivity distribution.

【0012】しかし、通常の条件、即ち第1コイル及び
第2コイルが同軸であり、且つ原料多結晶及び単結晶棒
もそれらと同軸という条件では、単結晶棒の断面内の電
気抵抗率分布は比較的大きく、必ずしも満足すべきもの
ではない。第2コイルを第1コイルに対して偏芯させ、
これに伴って単結晶棒を移動して第2コイルと単結晶が
同軸条件を保持した場合でも、単結晶の口径に応じ単結
晶棒の回転数及び偏芯量にある最適条件があることを本
発明者は研究の結果解明することができ、本発明に到達
した。
However, under normal conditions, that is, under the condition that the first coil and the second coil are coaxial and the raw material polycrystal and the single crystal rod are also coaxial with them, the electric resistivity distribution in the cross section of the single crystal rod becomes Relatively large, not always satisfactory. Decentering the second coil with respect to the first coil,
Accordingly, even when the single crystal rod is moved to maintain the coaxial condition between the second coil and the single crystal, there are optimal conditions for the rotation speed and the amount of eccentricity of the single crystal rod according to the diameter of the single crystal. The present inventors have been able to elucidate the results of the research and have reached the present invention.

【0013】FZ法による浮遊溶融帯域の攪拌は、温度
差による密度差自然対流、同じく表面張力の差にもとず
く表面張力対流、原料多結晶棒と単結晶棒との回転速度
差にもとずく攪拌、単結晶棒回転による遠心力による攪
拌、これに加えて偏芯による攪拌など、非常に複雑な要
素がからみあって上記溶融帯域の攪拌にどの要素が効く
かどうかは、実験をせずに予想出来るものではない。又
攪拌に遠心力が効果を有することは予想されるが、それ
は単結晶棒の口径も攪拌の一要因になることを意味す
る。
The agitation of the floating melting zone by the FZ method is based on the natural convection of the density difference due to the temperature difference, the convection of the surface tension based on the difference of the surface tension, and the rotation speed difference between the raw material polycrystalline rod and the single crystal rod. Without experimentation, it was not possible to determine which element would be effective in stirring the above-mentioned melting zone due to entanglement of extremely complex elements such as agitation, centrifugal stirring by rotation of a single crystal rod, and stirring by eccentricity. Not predictable. The centrifugal force is expected to have an effect on the stirring, which means that the diameter of the single crystal rod is also a factor of the stirring.

【0014】本発明は以上の複雑な要素の交絡したFZ
法単結晶製造装置における、単結晶棒断面内の不純物分
布即ち電気抵抗率分布とそれら諸要素との関係を詳細に
実施したところ、本発明の単結晶棒の口径、同回転数、
第1コイルと第2コイルの偏芯量が特別な数値範囲に維
持されることによって、最適条件たり得ることを知っ
た。
The present invention relates to an FZ in which the above complex elements are entangled.
In the method single crystal manufacturing apparatus, the impurity distribution in the cross section of the single crystal rod, that is, the electrical resistivity distribution and the relationship between the various elements were carried out in detail, the diameter of the single crystal rod of the present invention, the same rotation speed,
It has been found that the eccentricity of the first coil and the second coil is maintained in a special numerical range, so that the optimum condition can be obtained.

【0015】[0015]

【実施例】以下に本発明方法に用いられるFZ法単結晶
製造装置の一例を添付図面に基づいて概略的に説明す
る。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An example of an FZ method single crystal manufacturing apparatus used in the method of the present invention will be schematically described below with reference to the accompanying drawings.

【0016】図1は、FZ法単結晶製造装置2におい
て、本発明方法を実施する場合の第一コイル4及び第二
コイル6の配置を示す上面図である。図2は、図1の側
面図である。図3は、第一コイル4と第二コイル6の偏
芯位置及び原料多結晶8と単結晶10との偏芯位置との
関係を示す説明図である。第一コイル4の中心軸4aと
第二コイル6の中心軸6aのずれが偏芯量wである。な
お、8aは原料多結晶の中心軸、10aは単結晶の中心
軸である。12は電極である。
FIG. 1 is a top view showing the arrangement of the first coil 4 and the second coil 6 when the method of the present invention is performed in the FZ single crystal manufacturing apparatus 2. FIG. 2 is a side view of FIG. FIG. 3 is an explanatory diagram showing the relationship between the eccentric positions of the first coil 4 and the second coil 6 and the eccentric positions of the raw material polycrystal 8 and the single crystal 10. The deviation between the central axis 4a of the first coil 4 and the central axis 6a of the second coil 6 is the amount of eccentricity w. 8a is the central axis of the raw material polycrystal, and 10a is the central axis of the single crystal. 12 is an electrode.

【0017】上記装置を用いて、単結晶の口径と、単結
晶の回転数と、第一加熱コイルと第二加熱コイルの偏芯
量との関係を種々に変更して実験した例について説明す
る。
An example will be described in which the above-described apparatus is used to carry out various changes in the relationship among the diameter of the single crystal, the rotation speed of the single crystal, and the eccentricity of the first heating coil and the second heating coil. .

【0018】実験例1 口径2.5”のシリコン単結晶棒より、所定の位置から
厚さ300μmのウェーハを切取り面内に任意の直交す
る方向に2mmピッチで全点の電気抵抗率ρを4探針測
定法により測定し、最大値のρをρmax、最小値のρを
ρminとし、面内の電気抵抗変動率を次の式で定義し
た。
Experimental Example 1 A wafer having a thickness of 300 μm was cut from a predetermined position from a silicon single crystal rod having a diameter of 2.5 ″ into a cut plane, and the electrical resistivity ρ at all points was set to 4 at a pitch of 2 mm in an arbitrary orthogonal direction. The maximum value ρ was set to ρmax and the minimum value ρ was set to ρmin, and the in-plane electric resistance variation rate was defined by the following equation.

【0019】 [0019]

【0020】上記シリコン単結晶棒をFZ法で製造した
場合において、回転数(rpm)、偏芯量(mm)及び
RRG(%)の関係を調べて表1に示した。
Table 1 shows the relationship between the rotational speed (rpm), the amount of eccentricity (mm) and the RRG (%) when the silicon single crystal rod was manufactured by the FZ method.

【0021】[0021]

【表1】 [Table 1]

【0022】表1の結果から、口径2.5”の場合に良
好なRRGを得るための条件は、回転数が8〜30rp
mで偏芯量が6〜12mmであることが確認できた。な
お、RRGの良否の判定基準は、16%以下を良とし1
6%以上を否とした。
From the results shown in Table 1, the conditions for obtaining a good RRG when the diameter is 2.5 "are as follows.
m, the eccentricity was confirmed to be 6 to 12 mm. The criteria for determining the quality of the RRG is 1% or less and 1%.
6% or more was rejected.

【0023】実験例2 口径4”のシリコン単結晶棒について、実験例1と同様
に実験を行って、その結果を表2に示した。
Experimental Example 2 An experiment was performed on a silicon single crystal rod having a diameter of 4 ″ in the same manner as in Experimental Example 1, and the results are shown in Table 2.

【0024】[0024]

【表2】 [Table 2]

【0025】表2の結果から、口径4”の場合に良好な
RRGを得るための条件は、回転数が3〜12rpmで
偏芯量が4〜14mmであることが確認できた。なお、
RRGの良否の判定基準は、17%以下を良とし17%
以上を否とした。
From the results shown in Table 2, it was confirmed that the conditions for obtaining a good RRG in the case of a 4 "aperture were a rotational speed of 3 to 12 rpm and an eccentricity of 4 to 14 mm.
The criteria for determining the quality of RRG is 17% or less and 17%.
The above was rejected.

【0026】実験例3 口径5”のシリコン単結晶棒について、実験例1と同様
に実験を行って、その結果を表3に示した。
Experimental Example 3 An experiment was carried out on a silicon single crystal rod having a diameter of 5 ″ in the same manner as in Experimental Example 1, and the results are shown in Table 3.

【0027】[0027]

【表3】 [Table 3]

【0028】表3の結果から、口径5”の場合に良好な
RRGを得るための条件は、回転数が2〜6rpmで偏
芯量が3〜16mmであることが確認できた。なお、R
RGの良否の判定基準は、17%以下を良とし17%以
上を否とした。
From the results shown in Table 3, it was confirmed that the conditions for obtaining a good RRG in the case of a diameter of 5 ″ were a rotation speed of 2 to 6 rpm and an eccentricity of 3 to 16 mm.
The criterion for determining the quality of RG was 17% or less as good and 17% or more as bad.

【0029】実施例1 回転数3rpmで、偏芯量9mm(図1及び2に示した
二重コイルを用い、単結晶と多結晶の中心が9mmず
れ、同時に第1コイルと第2コイルも9mmずれる。)
として口径5”のシリコン単結晶棒を製造し、所定の位
置から厚さ300μmのウェーハを切取り面内に任意の
直交する方向に2mmピッチで電気抵抗値ρを測定し、
ウェーハの中心から円周方向の距離に対してプロットし
たプロファイルの1例を図4に示した。RRGは14.
91%であった。
Example 1 At a rotation speed of 3 rpm, the eccentricity was 9 mm (using the double coil shown in FIGS. 1 and 2, the center of the single crystal and the polycrystal were shifted by 9 mm, and simultaneously the first coil and the second coil were also 9 mm) It shifts.)
A silicon single crystal rod having a diameter of 5 ″ was manufactured, and an electric resistance value ρ was measured at an interval of 2 mm in an arbitrary orthogonal direction in a cut plane of a wafer having a thickness of 300 μm from a predetermined position,
One example of a profile plotted against the distance in the circumferential direction from the center of the wafer is shown in FIG. RRG is 14.
It was 91%.

【0030】比較例1 実施例と同じ装置において、第一コイルのみを設置し、
回転数3rpm、偏芯量9mm(単結晶と多結晶の中心
のずれが9mm)として口径5”のシリコン単結晶棒を
製造し、実施例1と同様に得たウェーハについての電気
抵抗値ρを測定して、図4と同様にしてプロファイルを
作成し、図5に示した。RRGは19.42%であっ
た。
Comparative Example 1 In the same apparatus as in the example, only the first coil was installed.
A silicon single crystal rod having a diameter of 5 ″ was manufactured at a rotation speed of 3 rpm and an eccentricity of 9 mm (a deviation between the center of a single crystal and a polycrystal was 9 mm). The measurement was made and a profile was created in the same manner as in Fig. 4, and shown in Fig. 5. The RRG was 19.42%.

【0031】[0031]

【発明の効果】以上述べたごとく、本発明のFZ法によ
る半導体シリコン単結晶の製造方法によれば、製造され
たシリコン単結晶棒断面内の電気抵抗分布のバラツキを
低減することができるという効果を奏する。
As described above, according to the method for producing a semiconductor silicon single crystal by the FZ method of the present invention, it is possible to reduce the variation of the electric resistance distribution in the cross section of the produced silicon single crystal rod. To play.

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

【図1】本発明方法を実施する場合の第一コイル及び第
二コイルの配置を示す上面図である。
FIG. 1 is a top view showing an arrangement of a first coil and a second coil when the method of the present invention is performed.

【図2】図1の側面図である。FIG. 2 is a side view of FIG.

【図3】第一コイルと第二コイルの偏芯位置及び原料多
結晶と単結晶との偏芯位置との関係を示す説明図であ
る。
FIG. 3 is an explanatory diagram showing a relationship between eccentric positions of a first coil and a second coil and eccentric positions of a raw material polycrystal and a single crystal.

【図4】本発明方法によって製造したシリコンウェーハ
についての電気抵抗値をウェーハ中心から円周方向の距
離に対してプロットしたプロファイルの1例を示すグラ
フである。
FIG. 4 is a graph showing an example of a profile in which the electric resistance value of a silicon wafer manufactured by the method of the present invention is plotted with respect to the distance in the circumferential direction from the center of the wafer.

【図5】従来方法によって製造したシリコンウェーハに
ついての電気抵抗値をウェーハ中心から円周方向の距離
に対してプロットしたプロファイルの1例を示すグラフ
である。
FIG. 5 is a graph showing one example of a profile in which electric resistance values of a silicon wafer manufactured by a conventional method are plotted with respect to a distance in a circumferential direction from a center of the wafer.

【符号の説明】[Explanation of symbols]

2 FZ法単結晶製造装置 4 第一コイル 4a 第一コイルの中心軸 6 第二コイル 6a 第二コイルの中心軸 8 原料多結晶 8a 原料多結晶の中心軸 10 単結晶 10a 単結晶の中心軸 2 FZ method single crystal manufacturing apparatus 4 First coil 4a Central axis of first coil 6 Second coil 6a Central axis of second coil 8 Raw material polycrystal 8a Central axis of raw material polycrystal 10 Single crystal 10a Central axis of single crystal

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 シリコン単結晶を高周波誘導加熱コイル
を用いて部分的に、加熱溶融しその溶融帯域を移動させ
ることによって単結晶成長を行うFZ法による半導体単
結晶製造方法に於いて、内側に位置する第一加熱コイル
と、外側に位置する第二加熱コイルを設置し該第一加熱
コイルの中心軸と原料多結晶の中心軸とを同軸にし、か
つ該第二加熱コイルの中心軸と単結晶の中心軸とを同軸
に配置し、かつ単結晶の口径によって単結晶の回転数及
び、第一加熱コイルと第二加熱コイルの偏芯量を選択す
ることを特徴とするFZ法による半導体シリコン単結晶
の製造方法。
In a method of manufacturing a semiconductor single crystal by an FZ method in which a silicon single crystal is partially heated and melted by using a high-frequency induction heating coil and a single crystal is grown by moving a melting zone thereof, A first heating coil is located, and a second heating coil is located on the outside, the central axis of the first heating coil and the central axis of the raw material polycrystal are made coaxial, and the central axis of the second heating coil is simply A semiconductor silicon according to the FZ method, wherein the central axis of the crystal is arranged coaxially, and the rotation speed of the single crystal and the amount of eccentricity of the first heating coil and the second heating coil are selected according to the diameter of the single crystal. Single crystal production method.
【請求項2】上記単結晶の口径と、単結晶の回転数と、
第一加熱コイルと第二加熱コイルの偏芯量との関係が次
の通りに設定することを特徴とする請求項1記載のFZ
法による半導体シリコン単結晶の製造方法。 口径 回転数rpm 偏芯量mm 2.5” 8〜30 6〜12 4.0” 3〜12 4〜14 5.0” 2〜6 3〜16
2. The diameter of the single crystal, the rotation speed of the single crystal,
2. The FZ according to claim 1, wherein the relationship between the eccentricity of the first heating coil and the eccentricity of the second heating coil is set as follows.
A method for producing a semiconductor silicon single crystal by a method. Diameter Rotation speed rpm Eccentricity mm 2.5 "8 to 30 6 to 12 4.0" 3 to 12 4 to 14 5.0 "2 to 6 3 to 16
JP3201348A 1991-07-16 1991-07-16 Method for producing semiconductor silicon single crystal by FZ method Expired - Lifetime JP2621069B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3201348A JP2621069B2 (en) 1991-07-16 1991-07-16 Method for producing semiconductor silicon single crystal by FZ method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3201348A JP2621069B2 (en) 1991-07-16 1991-07-16 Method for producing semiconductor silicon single crystal by FZ method

Publications (2)

Publication Number Publication Date
JPH0524966A JPH0524966A (en) 1993-02-02
JP2621069B2 true JP2621069B2 (en) 1997-06-18

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ID=16439549

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Application Number Title Priority Date Filing Date
JP3201348A Expired - Lifetime JP2621069B2 (en) 1991-07-16 1991-07-16 Method for producing semiconductor silicon single crystal by FZ method

Country Status (1)

Country Link
JP (1) JP2621069B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
BE1010771A3 (en) 1996-11-26 1999-01-05 Lhoist Rech & Dev Sa Soil treatment compositions, method of preparation and use.
CN109706521A (en) * 2017-10-25 2019-05-03 有研半导体材料有限公司 A method of zone melting single-crystal automatic growth is controlled according to growth angle
DE102018210317A1 (en) * 2018-06-25 2020-01-02 Siltronic Ag Method for producing a single crystal from semiconductor material according to the FZ method, device for carrying out the method and semiconductor wafer made of silicon

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4993202A (en) * 1973-01-10 1974-09-05
JPS539209A (en) * 1976-07-13 1978-01-27 Toshiba Corp High frequency heating coil of floating zone purifying apparatus
JPS542280A (en) * 1977-06-08 1979-01-09 Toyo Silicon Kk Preparation of semiconductor crystal by floating zone method
JPS63291887A (en) * 1987-05-25 1988-11-29 Shin Etsu Handotai Co Ltd Production device for semiconductor single crystal

Also Published As

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