JP2804456B2 - Method for growing Si single crystal with uniform impurity concentration distribution in radial direction - Google Patents
Method for growing Si single crystal with uniform impurity concentration distribution in radial directionInfo
- Publication number
- JP2804456B2 JP2804456B2 JP7091431A JP9143195A JP2804456B2 JP 2804456 B2 JP2804456 B2 JP 2804456B2 JP 7091431 A JP7091431 A JP 7091431A JP 9143195 A JP9143195 A JP 9143195A JP 2804456 B2 JP2804456 B2 JP 2804456B2
- Authority
- JP
- Japan
- Prior art keywords
- melt
- single crystal
- impurity concentration
- added
- radial direction
- 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 - Fee Related
Links
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- Crystals, And After-Treatments Of Crystals (AREA)
- Liquid Deposition Of Substances Of Which Semiconductor Devices Are Composed (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、半径方向に関する不純
物濃度分布が均一なSi単結晶を融液から育成する方法
に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for growing a Si single crystal having a uniform impurity concentration distribution in a radial direction from a melt.
【0002】[0002]
【従来の技術】融液からSi単結晶を育成する代表的な
方法として、チョクラルスキー法がある。チョクラルス
キー方法では、図1に示すように密閉容器1の内部に配
置したルツボ2を、回転及び昇降可能にサポート3で支
持する。ルツボ2の外周には、ヒータ4及び保温材5が
同心円状に設けられ、ルツボ2に収容した原料をヒータ
4で集中的に加熱し、融液6を調製する。融液6は、S
i単結晶成長に好適な温度に維持される。融液6に種結
晶7を接触させ、種結晶7の結晶方位を倣ったSi単結
晶8を成長させる。種結晶7は、ワイヤ9を介して回転
巻取り機構10又は剛性のある引き上げ棒から吊り下げ
られ、Si単結晶8の成長に応じて回転しながら引き上
げられる。また、ルツボ2も、サポート3を介して適宜
回転しながら下降する。サポート3の降下速度,回転速
度及び種結晶7の回転速度,上昇速度等は、融液6から
引上げられるSi単結晶8の成長速度に応じて制御され
る。2. Description of the Related Art A typical method for growing a Si single crystal from a melt is the Czochralski method. In the Czochralski method, a crucible 2 arranged inside a closed container 1 as shown in FIG. A heater 4 and a heat insulating material 5 are provided concentrically on the outer periphery of the crucible 2, and the raw material contained in the crucible 2 is intensively heated by the heater 4 to prepare a melt 6. Melt 6 is S
It is maintained at a temperature suitable for i-single crystal growth. The seed crystal 7 is brought into contact with the melt 6 to grow an Si single crystal 8 that follows the crystal orientation of the seed crystal 7. The seed crystal 7 is suspended from a rotary winding mechanism 10 or a rigid pulling rod via a wire 9, and is pulled while rotating in accordance with the growth of the Si single crystal 8. The crucible 2 also descends while rotating appropriately via the support 3. The lowering speed and rotating speed of the support 3 and the rotating speed and rising speed of the seed crystal 7 are controlled according to the growth speed of the Si single crystal 8 pulled from the melt 6.
【0003】[0003]
【発明が解決しようとする課題】融液6には、Si単結
晶8に種々の要求特性を付与するため、各種の不純物が
添加される。しかし、添加された不純物の種類によって
は、成長界面における融液の挙動が異なってくるものも
ある。なかでも、Ga,Sb等の不純物を添加したSi
融液は、融液撹拌効果が減少し易く、それに伴って半径
方向に関する不純物分布が不均一になる。本発明者等
は、不純物濃度が不均一になる原因を次のように推察し
た。すなわち、Ga又はSbを添加した融液は、熱膨張
係数が融点近傍で約6.0×10-6/℃となり、熱膨張
係数に依存した乱流効果が低下する。そのため、添加不
純物が十分に撹拌されず、結果として成長界面直下で半
径方向に関する不純物濃度が不均一化する。不均一な不
純物濃度分布は、界面直下に形成される不純物境界層に
そのまま保存され、結晶中に取り込まれる。その結果、
引き上げられたSi単結晶の不純物濃度が半径方向に関
して不安定化し、得られたSi単結晶の品質安定性を低
下させる。本発明は、このような問題を解消すべく案出
されたものであり、熱膨張係数を大きくする元素をSi
融液に追加添加することにより、成長界面直下で融液を
拡散する作用を向上させ、半径方向に関して不純物濃度
が均一化された高品質のSi単結晶を得ることを目的と
する。Various impurities are added to the melt 6 in order to impart various required characteristics to the Si single crystal 8. However, depending on the type of impurity added, the behavior of the melt at the growth interface may be different. Among them, Si doped with impurities such as Ga and Sb
In the melt, the effect of stirring the melt is easily reduced, and accordingly, the impurity distribution in the radial direction becomes non-uniform. The present inventors presumed the cause of the non-uniform impurity concentration as follows. That is, the melt to which Ga or Sb is added has a thermal expansion coefficient of about 6.0 × 10 −6 / ° C. near the melting point, and the turbulence effect depending on the thermal expansion coefficient is reduced. Therefore, the added impurities are not sufficiently stirred, and as a result, the impurity concentration in the radial direction immediately below the growth interface becomes uneven. The non-uniform impurity concentration distribution is preserved as it is in the impurity boundary layer formed immediately below the interface, and is taken into the crystal. as a result,
The impurity concentration of the pulled Si single crystal becomes unstable in the radial direction, and the quality stability of the obtained Si single crystal is reduced. The present invention has been devised to solve such a problem, and an element for increasing the thermal expansion coefficient is made of Si.
It is an object of the present invention to improve the effect of diffusing the melt immediately below the growth interface by additionally adding to the melt, and to obtain a high-quality Si single crystal having a uniform impurity concentration in the radial direction.
【0004】[0004]
【課題を解決するための手段】本発明のSi単結晶育成
方法は、その目的を達成するため、Ga又はSbを添加
したSi融液からチョクラルスキー法でSi単結晶を引
き上げる際、周期律表でGa又はSbと同じグループに
属し、融点近傍における前記融液の熱膨張係数を大きく
する元素を前記融液に追加添加することを特徴とする。
熱膨張係数を大きくする元素としてはB又はPがあり、
Ga添加Si融液に対してはBが、Sb添加Si融液に
対してはPが追加添加される。これら追加添加される元
素は、添加元素(Ga又はSb)と周期律表上で属する
グループ(III又はIV族)が一致し、添加後の抵抗値が
0.001〜10Ω・cmとなるものとして添加され、
結晶育成中に融液表面における蒸発を考慮すると1×1
018〜5×1020原子/cm3 の範囲に添加量が定めら
れる。According to the method for growing a Si single crystal of the present invention, when a Si single crystal is pulled up from a Si melt to which Ga or Sb is added by the Czochralski method, a periodic rule is set. An element that belongs to the same group as Ga or Sb in the table and that increases the thermal expansion coefficient of the melt near the melting point is additionally added to the melt.
Elements that increase the coefficient of thermal expansion include B and P,
B is added to the Ga-added Si melt, and P is added to the Sb-added Si melt. These additional elements are such that the added element (Ga or Sb) matches the group (group III or IV) belonging to the periodic table and the resistance value after addition becomes 0.001 to 10 Ω · cm. Added
Considering evaporation on the melt surface during crystal growth, 1 × 1
The addition amount is determined in the range of 0 18 to 5 × 10 20 atoms / cm 3 .
【0005】[0005]
【作用】Si融液から引き上げられた単結晶の半径方向
に関する不純物濃度分布の不均一性は、成長界面直下に
おける融液の不純物濃度分布の均一性に依存している。
したがって、半径方向に関する不純物濃度分布を均一化
するためには、成長界面直下において融液の撹拌を活発
化させる必要がある。本発明者等の研究によるとき、融
液の熱膨張を増加させるB,P等の元素を添加すると、
成長界面直下で融液の撹拌が促進されることを見い出し
た。すなわち、B,P等の元素を添加した融液は、凝固
点近傍にある成長界面直下で熱膨張が局部的に大きくな
る。そのため、周囲にある融液との間で熱膨張差が大き
くなり、熱膨張差に起因して融液の循環流動が加速され
る。その結果、成長界面直下の融液が十分な撹拌作用を
受け、半径方向に関する不純物濃度分布が均一化され
る。したがって、この融液から引上げられたSi単結晶
は、半径方向に関して不純物濃度分布が均一化された高
品質の結晶となる。The non-uniformity of the impurity concentration distribution in the radial direction of the single crystal pulled from the Si melt depends on the uniformity of the impurity concentration distribution of the melt immediately below the growth interface.
Therefore, in order to make the impurity concentration distribution uniform in the radial direction, it is necessary to activate the stirring of the melt immediately below the growth interface. According to the study of the present inventors, when elements such as B and P which increase the thermal expansion of the melt are added,
It has been found that stirring of the melt is promoted immediately below the growth interface. That is, the melt to which elements such as B and P are added has a locally large thermal expansion just below the growth interface near the freezing point. Therefore, the difference in thermal expansion between the melt and the surrounding melt is increased, and the circulating flow of the melt is accelerated due to the difference in thermal expansion. As a result, the melt immediately below the growth interface receives a sufficient stirring action, and the impurity concentration distribution in the radial direction is made uniform. Therefore, the Si single crystal pulled from the melt becomes a high-quality crystal having a uniform impurity concentration distribution in the radial direction.
【0006】[0006]
【実施例】Ga又はSbを0.1原子%添加したSi原
料5kgに、更にB又はPを1015原子/cm3 添加
し、ルツボで溶解した。そして、単結晶引上げ開始まで
の間、アルゴンガスを充満したチャンバー内にSi融液
を保持した。Ga又はSbを添加した融液は、図2に示
す密度の温度依存性から、融点〜1430℃の温度域に
おける熱膨張係数が約6.0×10-6/℃と推定され
る。特に、融点〜1430℃の温度域では密度の急激な
変動が緩和され、十分な撹拌作用が得られず、融液中の
不純物分布が均質であることが伺われる。この融液に更
にB又はPを添加したものでは、図2に示す0.1原子
%B又はPを添加した密度の温度依存性から、融点〜1
430℃の温度域における熱膨張係数が約1.5×10
-3/℃と推定される。すなわち、Ga又はSbを添加し
たときに比べて、その熱膨張係数が増加することが予想
され、融液に循環流動が活発になる。EXAMPLE B or P was further added at 10 15 atoms / cm 3 to 5 kg of a Si raw material to which 0.1 atomic% of Ga or Sb was added, and was dissolved in a crucible. Then, the Si melt was held in a chamber filled with argon gas until the start of pulling the single crystal. From the temperature dependence of the density shown in FIG. 2, the melt to which Ga or Sb is added is estimated to have a thermal expansion coefficient of about 6.0 × 10 −6 / ° C. in a temperature range from the melting point to 1430 ° C. In particular, in the temperature range from the melting point to 1430 ° C., the rapid fluctuation of the density is alleviated, a sufficient stirring action cannot be obtained, and it is apparent that the impurity distribution in the melt is uniform. In the case where B or P was further added to this melt, the melting point to 1 point was obtained from the temperature dependency of the density of adding 0.1 atomic% B or P shown in FIG.
The thermal expansion coefficient in the temperature range of 430 ° C. is about 1.5 × 10
-3 / ° C. That is, the thermal expansion coefficient is expected to increase as compared with the case where Ga or Sb is added, and the circulating flow in the melt becomes active.
【0007】実際にGaドープSi融液及びGa,Bド
ープSi融液それぞれから直径3インチ及び長さ200
mmのSi単結晶を引き上げ、成長方向に関する不純物
濃度を測定した。測定結果を示す図3にみられるよう
に、GaドープSi融液にBを添加しない場合は、半径
方向の抵抗率の変動が±20%であった。これに対し
て、Bを更に添加した場合は、抵抗率の変動が±5%の
範囲に抑えられている。この対比から明らかなように、
熱膨張係数を大きくする元素を添加することによって、
成長界面直下で十分な融液の撹拌が確保され、半径方向
に関して不純物濃度分布が均一化されたSi単結晶が得
られることが確認された。[0007] Actually, each of the Ga-doped Si melt and the Ga, B-doped Si melt has a diameter of 3 inches and a length of 200 mm.
mm single crystal was pulled up, and the impurity concentration in the growth direction was measured. As shown in FIG. 3 showing the measurement results, when B was not added to the Ga-doped Si melt, the variation in the resistivity in the radial direction was ± 20%. On the other hand, when B was further added, the variation in resistivity was suppressed to a range of ± 5%. As is clear from this contrast,
By adding an element that increases the coefficient of thermal expansion,
It was confirmed that sufficient stirring of the melt was ensured immediately below the growth interface, and that a Si single crystal having a uniform impurity concentration distribution in the radial direction was obtained.
【0008】[0008]
【発明の効果】以上に説明したように、本発明において
は、熱膨張係数を大きくする元素を添加したGa又はS
bドープSi融液から、チョクラルスキー法によってS
i単結晶を育成している。熱膨張係数を大きくする元素
は、成長界面直下で融液を十分に撹拌する作用を呈し、
不純物濃度分布が均一化された融液から単結晶が育成さ
れることを可能にする。そのため、得られたSi単結晶
は、半径方向に関して不純物濃度分布が均一化した高品
質の単結晶となる。As described above, in the present invention, Ga or S doped with an element which increases the coefficient of thermal expansion is used.
From the b-doped Si melt, S
Growing i single crystal. The element that increases the coefficient of thermal expansion has the effect of sufficiently stirring the melt just below the growth interface,
A single crystal can be grown from a melt having a uniform impurity concentration distribution. Therefore, the obtained Si single crystal is a high-quality single crystal having a uniform impurity concentration distribution in the radial direction.
【図1】 融液からSi単結晶を引き上げるチョクラル
スキー法Fig. 1 Czochralski method for pulling a Si single crystal from a melt
【図2】 各種不純物を添加したSi融液の密度と温度
との関係を示すグラフFIG. 2 is a graph showing the relationship between the density and temperature of a Si melt to which various impurities are added.
【図3】 引き上げられたSi単結晶の成長方向に関す
る不純物濃度分布を抵抗値で表したグラフFIG. 3 is a graph showing an impurity concentration distribution in a growth direction of a pulled Si single crystal by a resistance value.
1:密閉容器 2:ルツボ 3:サポート 4:
ヒータ 5:保温材 6:融液 7:種結晶 8:Si単結晶 9:ワ
イヤ 10:回転巻取り機構1: Closed container 2: Crucible 3: Support 4:
Heater 5: Insulation material 6: Melt 7: Seed crystal 8: Si single crystal 9: Wire 10: Rotary winding mechanism
───────────────────────────────────────────────────── フロントページの続き (73)特許権者 000006264 三菱マテリアル株式会社 東京都千代田区大手町1丁目5番1号 (73)特許権者 000205351 住友シチックス株式会社 兵庫県尼崎市東浜町1番地 (72)発明者 川西 荘六 茨城県つくば市東光台1−16−2 (72)発明者 泉妻 宏治 茨城県稲敷郡阿見町荒川沖1770−1− 502 (72)発明者 十河 慎二 茨城県つくば市今鹿島4182−3 (72)発明者 佐々木 斉 埼玉県大宮市大成町1−545 (72)発明者 木村 茂行 茨城県つくば市竹園3−712 (72)発明者 碇 敦 茨城県つくば市東光台2−12−15 (56)参考文献 特開 昭57−118089(JP,A) 特開 平6−204150(JP,A) 特開 昭62−226890(JP,A) KAWANISHI S.ET A L.,”EFFECT OF IMPU RITY DOPING ON DEN SITY ANOMALIES INM OLTEN SILICON”,JP N.J.APPL.PHYS.PART 2,JAPAN,15 NOV.1995, VOL.34,NO.11B,PP.L1509 −1512 KAWANISHI S.ET A L.,”EFFECT OF GALL IUM ADDITION ON DE NSITY VARIATION OF MOLTEN SILICON”,J PN.J.APPL.PHYS.PAR T 1,JAPAN,FEB.1995,V OL.34,NO.2A,PP.482−483 (58)調査した分野(Int.Cl.6,DB名) C30B 29/06 C30B 15/04 H01L 21/208────────────────────────────────────────────────── ─── Continuing on the front page (73) Patent holder 000006264 Mitsubishi Materials Corporation 1-5-1, Otemachi, Chiyoda-ku, Tokyo (73) Patent holder 000205351 Sumitomo Sitix Corporation 1-Higashihama-cho, Amagasaki-shi, Hyogo (72 Inventor Soroku Kawanishi 1-16-2 Tokodai, Tsukuba, Ibaraki Pref. (72) Inventor Koji Izuma, 1770-1-502 off Arakawa, Ami-cho, Inashiki-gun, Ibaraki Pref. 4182-3 Kashima (72) Inventor Hitoshi Sasaki 1-545, Taiseicho, Omiya City, Saitama Prefecture (72) Inventor Shigeyuki Kimura 3-712 Takezono, Tsukuba City, Ibaraki Prefecture (72) Inventor Atsushi Ikari 2- Tokodai, Tsukuba City, Ibaraki Prefecture 12-15 (56) References JP-A-57-118089 (JP, A) JP-A-6-204150 (JP, A) JP-A-62-226890 (JP, A) KAWANISHI S. ET AL. , "EFFECT OF IMPU RITY DOPING ON DEN SITY ANOMALLIES INM OLTEN SILICON", JPN. J. APPL. PHYS. PART 2, JAPAN, 15 NOV. 1995, VOL. 34, NO. 11B, PP. L1509-1512 KAWANISHI S.L. ET AL. , "EFFECT OF GALL IUM ADDITION ON DE NITY VARIATION OF MOLTEN SILICON", JPN. J. APPL. PHYS. PAR T 1, JAPAN, FEB. 1995, VOL. 34, NO. 2A, PP. 482-483 (58) Fields surveyed (Int.Cl. 6 , DB name) C30B 29/06 C30B 15/04 H01L 21/208
Claims (2)
スキー法でSi単結晶を引き上げる際、融点近傍におけ
る前記融液の熱膨張係数を大きくするBを前記融液に追
加添加することを特徴とする温度変動を抑制したSi単
結晶の育成方法。 Czochral from a Si melt to which Ga is added.
When pulling the Si single crystal by the ski method,
B, which increases the coefficient of thermal expansion of the melt, is added to the melt.
A method for growing a Si single crystal in which temperature fluctuation is suppressed, characterized by additionally adding .
スキー法でSi単結晶を引き上げる際、融点近傍におけ
る前記融液の熱膨張係数を大きくするPを前記融液に追
加添加することを特徴とする温度変動を抑制したSi単
結晶の育成方法。2. Czochral from a Si melt to which Sb has been added.
When pulling the Si single crystal by the ski method,
P, which increases the thermal expansion coefficient of the melt, is added to the melt.
A method for growing a Si single crystal in which temperature fluctuation is suppressed, characterized by additionally adding .
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7091431A JP2804456B2 (en) | 1995-03-24 | 1995-03-24 | Method for growing Si single crystal with uniform impurity concentration distribution in radial direction |
| EP96104454A EP0733726A3 (en) | 1995-03-24 | 1996-03-20 | Growth of a silicon single crystal having a uniform longitudinal or radial distribution of impurities |
| US08/620,391 US5700320A (en) | 1995-03-24 | 1996-03-22 | Growth of silicon single crystal having uniform impurity distribution along lengthwise or radial direction |
| KR1019960008023A KR100264399B1 (en) | 1995-03-24 | 1996-03-23 | Growth of silicon single crystal having uniform impurity distribution along lengthwise direction |
| KR1020000009606A KR100269088B1 (en) | 1995-03-24 | 2000-02-26 | Growth of silicon single crystal having uniform impurity distribution along radial direction |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7091431A JP2804456B2 (en) | 1995-03-24 | 1995-03-24 | Method for growing Si single crystal with uniform impurity concentration distribution in radial direction |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH08259374A JPH08259374A (en) | 1996-10-08 |
| JP2804456B2 true JP2804456B2 (en) | 1998-09-24 |
Family
ID=14026189
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7091431A Expired - Fee Related JP2804456B2 (en) | 1995-03-24 | 1995-03-24 | Method for growing Si single crystal with uniform impurity concentration distribution in radial direction |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2804456B2 (en) |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE3049376A1 (en) * | 1980-12-29 | 1982-07-29 | Heliotronic Forschungs- und Entwicklungsgesellschaft für Solarzellen-Grundstoffe mbH, 8263 Burghausen | METHOD FOR PRODUCING VERTICAL PN TRANSITIONS WHEN DRAWING SILICO DISC FROM A SILICONE MELT |
| JPH06204150A (en) * | 1992-12-28 | 1994-07-22 | Sumitomo Sitix Corp | Manufacture of silicon single crystal substrate for semiconductor |
-
1995
- 1995-03-24 JP JP7091431A patent/JP2804456B2/en not_active Expired - Fee Related
Non-Patent Citations (2)
| Title |
|---|
| KAWANISHI S.ET AL.,"EFFECT OF GALLIUM ADDITION ON DENSITY VARIATION OF MOLTEN SILICON",JPN.J.APPL.PHYS.PART 1,JAPAN,FEB.1995,VOL.34,NO.2A,PP.482−483 |
| KAWANISHI S.ET AL.,"EFFECT OF IMPURITY DOPING ON DENSITY ANOMALIES INMOLTEN SILICON",JPN.J.APPL.PHYS.PART 2,JAPAN,15 NOV.1995,VOL.34,NO.11B,PP.L1509−1512 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH08259374A (en) | 1996-10-08 |
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