JPH0351673B2 - - Google Patents
Info
- Publication number
- JPH0351673B2 JPH0351673B2 JP60173940A JP17394085A JPH0351673B2 JP H0351673 B2 JPH0351673 B2 JP H0351673B2 JP 60173940 A JP60173940 A JP 60173940A JP 17394085 A JP17394085 A JP 17394085A JP H0351673 B2 JPH0351673 B2 JP H0351673B2
- Authority
- JP
- Japan
- Prior art keywords
- crystal
- crucible
- magnetic field
- melt
- single crystal
- 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
Links
Landscapes
- Liquid Deposition Of Substances Of Which Semiconductor Devices Are Composed (AREA)
- Crystals, And After-Treatments Of Crystals (AREA)
Description
〔産業上の利用分野〕
本発明は、引上げ法によるSiやGaAsなどの半
導体あるいは無機化合物などの単結晶の製造方法
およびその装置に関する。
〔従来の技術〕
引上げ法はチヨクラルスキー法とも言われ、大
径の単結晶インゴツトが得やすいなどの利点があ
るためSiやGaAsなどの単結晶の製造に実用され
ている。しかしながら、酸素不純物濃度が高いこ
と、ストリエーシヨンと呼ばれる縞状の欠陥(成
長縞)が発生するなどの欠点があつた。
これらの欠点を解決するため、例えば特公昭58
−50953では、ルツボ中の溶融Siに静磁場を印加
し、該溶融Siの流動を抑制することが提案されて
いる。Si中の酸素の固液平衡分配係数は1.25と1
より大きいので、引上げ中の単結晶と接するSi融
液の酸素濃度は、第2図に示すように母液相の濃
度より低くなる。従つて、溶融Siの流動を抑制す
ることにより、母液相から、固/液界面に運ばれ
る酸素の量を減らせば、単結晶中の酸素濃度が減
少する。さらに、溶融Siの流動を抑制するとルツ
ボに使用するSiO2から溶融Siへの酸素の溶出も
減少する。以上、2つの効果により単結晶インゴ
ツト中の酸素濃度が減少すると考えられている。
一方、特開昭59−131597においては、GaAs単
結晶をチヨクラルスキー法で製造する際、静磁場
を印加することにより成長縞の無い高品質の結晶
を得ている。
さらに、特開昭55−10405ではSi融液に回転磁
界を与え、該Si融液を回転することが提案されて
いる。
Japanese Journal of Appied Physics、vol
19(1980)p.p.L−33〜36に発表された実験結果に
よると、単結晶インゴツトを、上記Si融液の回転
と同一方向に回転すると酸素濃度は減少し、さら
にルツボをもSi融液の回転と同一方向に回転する
と一層酸素濃度が減少する。単結晶インゴツトと
ルツボの回転方向と同一方向にSi融液を回転させ
ると、Si融液が、単結晶インゴツトとルツボに対
し、相対的に静止していることになるため、静磁
場印加法と同様の効果が得られるものと考えられ
る。
さて、チヨクラルスキー法においては、単結晶
インゴツトを回転しながら引上げる。この目的の
1つは、該インゴツト水平面内のドーピング元素
濃度を均一にすることである。第2図に示すよう
に、PやBなどのドーピング元素は固液分配係数
が1より小さいため、酸素とは逆に固/液界面の
濃度が母液相濃度より高くなる。このPやBの
固/液界面濃度は、凝固に伴う排出速度と母液相
への拡散速度のかねあいで決まる。
結晶を回転しない場合には、第3図に示すよう
な熱対流10が発生し、この洗浄効果により拡散
が促進され、結晶側面近くは中心部に比べてPや
Bの界面の濃度が低くなる。単結晶インゴツトを
回転すると第4図に示すように結晶中心部にSi融
液の上昇流(強制対流11)を生じ中心部でのP
やBの濃度を端部のそれと同程度にする効果があ
る。それ故、結晶回転による強制対流によりイン
ゴツト水平面内のドーピング元素濃度が均一化す
る効果がある。
SiやGaAs融液に静磁場を印加すると熱対流1
1のみでなく、上記のように有用な働きをする強
制対流をも抑制する。また、回転磁場によりSi融
液をSi融液と同方向に回転させる場合も第4図に
示す強制対流は弱められる。この結果、静磁場や
回転磁場を印加すると、インゴツト面内のドーピ
ング元素濃度の分布が不均一性を増大するという
欠点があつた。
〔発明が解決しようとする問題点〕
本発明は、単結晶面内のドーピング元素や不純
物元素などの不均一などの弊害をもたらすことな
く、またルツボ材のSiO2からSi融液中へ酸素が
溶出するのを低減することを目的とする。
〔問題点を解決するための手段〕
本発明者らは、結晶回転による強制対流を減ず
ることなく、熱対流のみを防止する方法につき
種々検討した結果、本発明を知見するに至つた。
本発明は、ルツボ内融液に下向きの進行磁場を
印加することにより該融液内の熱対流を防止し、
これによつてルツボ材の溶出を低減するものであ
つて、溶融物質から引上げ法にて単結晶を製造す
る方法において、収容容器内のルツボ側壁近傍の
溶融物質に下向きの進行磁場を印加しながら種結
晶を引上げることにより結晶成長を行うことを特
徴とする。
また本発明の装置は上記方法の実施のために専
ら用いる装置であつて、
(a) 加熱装置を備え溶融物質を収容する単結晶引
上げ用容器、
(b) 該容器の側壁の外周を取囲んで設けられ容器
内の溶融物質に下向きの進行磁場を印加する手
段、
を設けたことを特徴とする単結晶の製造装置であ
る。
進行磁場を印加する手段は、溶融物質収納容器
の側壁を取囲む電磁石と、これに低周波交流電流
を供給する装置とから成る。
〔作用〕
電導性の液体に進行磁場を印加すると、誘起電
流と磁場との相互作用により該液体に流動の駆動
力を与えることができ、この原理は、流体輸送用
の電磁ポンプなどに用いられている。この際、電
流が誘起される範囲すなわち、浸透深さδは次式
で表わされる。
δ=(1/πfμσ)1/2 ……(1)
ここに、μ:透磁率
σ:電導率
である。
上記進行磁場の振動数fが増大するにつれて浸
透深さδは減少する。
従つて、目的に応じて適切な振動数を選択する
ことにより浸透深さδ、言い換えると流動の駆動
力の及ぶ範囲を変えることができる。
第1図は本発明の装置の構成を示したものであ
り、ルツボ3の側壁を取囲むように、チエンバ外
壁2の外側に進行磁場発生用の電磁石1を設置す
る。この電磁石1は立設円筒形として、ルツボ内
Si融液4に軸対称の進行磁場を与える。
ルツボ3内のSi融液は、ヒータ6によりルツボ
3を介して熱せられているために、ルツボ側壁近
傍のSi融液の温度が内部より高くなり、この温度
差による浮力により第3図、第4図に示す熱対流
10が発生する。本発明は進行磁場により、ルツ
ボ側壁近傍のSi融液に、上記浮力に抗する下向き
の力を与えることにより熱対流10を抑止する。
〔実施例〕
次に本発明の実施例につき詳しく説明する。
実施例 1
第1図に示す装置を用いてSi単結晶の引上げを
行つた。この装置はルツボ3内にSi融液4を収納
し、この融液から単結晶5を引上げる。ルツボ3
の外周にヒータ6、その外周に熱シールド7を備
え、これらはチエンバ外壁2で被覆されている。
このチエンバ外壁2の外周に、ルツボ3の側壁の
周囲を取囲むように電磁石1が設けられる。電磁
石1には図示しない低周波発振装置から進行磁場
を発生する交流電流が供給される。
本発明の実施例においては、ルツボ内融液に、
ルツボ側壁部で磁場強度100ガウス、周波数100Hz
の下向きの進行磁場を印加した。また、比較例に
おいては、同装置を用い、磁場印加をせずに引上
げを行つた。実施例、比較例共に、結晶およびル
ツボの回転数はそれぞれ20rpmおよび10rpm逆向
きとした。
単結晶インゴツトの頭部付近から切り出して製
造したSiウエハにつき、実施例と比較例の特性比
較を行つた。その結果を第1表に示す。
実施例は、比較例に比べ酸素濃度が約1/4に
減少した。これは、熱対流の抑制により、ルツボ
材のシリカからの酸素の溶出が減少した効果と考
えられる。一方、実施例と比較例でウエハ面内の
抵抗値ばらつきは同じである。
以上のように本発明により、ウエハ面内のドー
ピング元素分布、言い換えると抵抗値分布の不均
一性を増すことなく、酸素濃度を大幅に低減する
ことができる。
[Industrial Application Field] The present invention relates to a method for producing a single crystal of a semiconductor such as Si or GaAs or an inorganic compound by a pulling method, and an apparatus therefor. [Prior Art] The pulling method is also called the Czyochralski method, and it is used in the production of single crystals such as Si and GaAs because it has advantages such as the ease of obtaining large-diameter single crystal ingots. However, there were drawbacks such as a high concentration of oxygen impurities and the occurrence of striped defects (growth stripes) called striations. In order to solve these shortcomings, for example,
-50953 proposes applying a static magnetic field to molten Si in a crucible to suppress the flow of the molten Si. The solid-liquid equilibrium partition coefficient of oxygen in Si is 1.25 and 1
Therefore, the oxygen concentration of the Si melt in contact with the single crystal being pulled is lower than the concentration of the mother liquid phase, as shown in FIG. Therefore, by suppressing the flow of molten Si and reducing the amount of oxygen transported from the mother liquid phase to the solid/liquid interface, the oxygen concentration in the single crystal will be reduced. Furthermore, suppressing the flow of molten Si also reduces the elution of oxygen from SiO 2 used in the crucible to molten Si. It is believed that the oxygen concentration in the single crystal ingot decreases due to the above two effects. On the other hand, in Japanese Patent Application Laid-Open No. 59-131597, when a GaAs single crystal is manufactured by the Czyochralski method, a high quality crystal without growth striations is obtained by applying a static magnetic field. Furthermore, Japanese Patent Laid-Open No. 10405/1983 proposes applying a rotating magnetic field to the Si melt to rotate the Si melt. Japanese Journal of Applied Physics, vol.
19 (1980) ppL-33-36, the oxygen concentration decreases when a single crystal ingot is rotated in the same direction as the rotation of the Si melt, and the crucible is also rotated in the same direction as the rotation of the Si melt. When rotating in the same direction, the oxygen concentration decreases further. If the Si melt is rotated in the same direction as the rotation direction of the single crystal ingot and the crucible, the Si melt will remain stationary relative to the single crystal ingot and the crucible. It is thought that similar effects can be obtained. Now, in the Czyochralski method, a single crystal ingot is pulled up while rotating. One purpose of this is to make the doping element concentration uniform in the horizontal plane of the ingot. As shown in FIG. 2, since doping elements such as P and B have solid-liquid partition coefficients smaller than 1, the concentration at the solid/liquid interface becomes higher than the mother liquid phase concentration, contrary to oxygen. The solid/liquid interface concentration of P and B is determined by the balance between the discharge rate accompanying solidification and the diffusion rate into the mother liquid phase. If the crystal is not rotated, thermal convection 10 as shown in Figure 3 occurs, and this cleaning effect promotes diffusion, resulting in a lower concentration of P and B at the interface near the sides of the crystal than in the center. . When a single crystal ingot is rotated, an upward flow of Si melt (forced convection 11) is generated in the center of the crystal, as shown in Figure 4, and P is increased in the center.
This has the effect of making the concentration of B and B similar to that at the end. Therefore, forced convection caused by crystal rotation has the effect of making the doping element concentration uniform in the horizontal plane of the ingot. When a static magnetic field is applied to Si or GaAs melt, thermal convection 1
1, but also suppresses forced convection, which plays a useful role as described above. Also, when the Si melt is rotated in the same direction as the Si melt by a rotating magnetic field, the forced convection shown in FIG. 4 is weakened. As a result, when a static magnetic field or a rotating magnetic field is applied, there is a drawback that the distribution of doping element concentration within the ingot surface becomes non-uniform. [Problems to be Solved by the Invention] The present invention eliminates the problem of non-uniformity of doping elements and impurity elements within a single crystal plane, and also allows oxygen to be transferred from SiO 2 of the crucible material into the Si melt. The purpose is to reduce elution. [Means for Solving the Problems] The present inventors have studied various methods for preventing only thermal convection without reducing forced convection due to crystal rotation, and as a result, have discovered the present invention. The present invention prevents thermal convection within the melt by applying a downward traveling magnetic field to the melt in the crucible,
This reduces the elution of the crucible material, and in the method of manufacturing single crystals from molten material by the pulling method, while applying a downward traveling magnetic field to the molten material near the side wall of the crucible in the storage container. It is characterized by crystal growth by pulling up a seed crystal. Furthermore, the apparatus of the present invention is an apparatus exclusively used for carrying out the above method, and includes (a) a single crystal pulling container equipped with a heating device and containing a molten substance, and (b) a container surrounding the outer periphery of the side wall of the container. A device for producing a single crystal, comprising means for applying a downward traveling magnetic field to a molten substance in a container. The means for applying a traveling magnetic field consists of an electromagnet surrounding the side wall of the molten material container and a device for supplying it with a low frequency alternating current. [Operation] When a traveling magnetic field is applied to an electrically conductive liquid, the interaction between the induced current and the magnetic field can provide a driving force for the liquid to flow. This principle is used in electromagnetic pumps for fluid transport, etc. ing. At this time, the range in which the current is induced, that is, the penetration depth δ is expressed by the following equation. δ=(1/πfμσ) 1/2 ...(1) where μ: magnetic permeability σ: electrical conductivity. As the frequency f of the traveling magnetic field increases, the penetration depth δ decreases. Therefore, by selecting an appropriate frequency according to the purpose, the penetration depth δ, in other words, the range of the flow driving force can be changed. FIG. 1 shows the configuration of the apparatus of the present invention, in which an electromagnet 1 for generating a traveling magnetic field is installed outside the chamber outer wall 2 so as to surround the side wall of the crucible 3. This electromagnet 1 is installed in an upright cylindrical shape inside the crucible.
An axially symmetrical traveling magnetic field is applied to the Si melt 4. Since the Si melt in the crucible 3 is heated by the heater 6 via the crucible 3, the temperature of the Si melt near the side wall of the crucible becomes higher than that inside the crucible, and due to the buoyancy caused by this temperature difference, as shown in FIG. Heat convection 10 shown in FIG. 4 occurs. The present invention suppresses thermal convection 10 by applying a downward force against the buoyant force to the Si melt near the side wall of the crucible using a traveling magnetic field. [Example] Next, an example of the present invention will be described in detail. Example 1 A Si single crystal was pulled using the apparatus shown in FIG. This device stores a Si melt 4 in a crucible 3 and pulls a single crystal 5 from this melt. Crucible 3
A heater 6 is provided on the outer periphery of the chamber, and a heat shield 7 is provided on the outer periphery of the chamber, and these are covered with the chamber outer wall 2.
An electromagnet 1 is provided on the outer periphery of the chamber outer wall 2 so as to surround the side wall of the crucible 3. The electromagnet 1 is supplied with an alternating current that generates a traveling magnetic field from a low frequency oscillator (not shown). In the embodiment of the present invention, the melt in the crucible contains
Magnetic field strength 100 Gauss, frequency 100Hz at crucible side wall
A downward traveling magnetic field was applied. Furthermore, in a comparative example, the same device was used to perform pulling without applying a magnetic field. In both Examples and Comparative Examples, the rotation speeds of the crystal and crucible were 20 rpm and 10 rpm, respectively, in opposite directions. The characteristics of the example and the comparative example were compared for Si wafers manufactured by cutting out the vicinity of the head of a single crystal ingot. The results are shown in Table 1. In the example, the oxygen concentration was reduced to about 1/4 compared to the comparative example. This is thought to be due to the effect that the elution of oxygen from the silica of the crucible material was reduced due to the suppression of thermal convection. On the other hand, the resistance value variation within the wafer surface is the same between the example and the comparative example. As described above, according to the present invention, the oxygen concentration can be significantly reduced without increasing the non-uniformity of the doping element distribution within the wafer surface, in other words, the resistance value distribution.
本発明により、パワートランジスタ用などに必
要な低酸素濃度のシリコンウエハを引上げ結晶を
用いて製造することができる。また、本発明法に
よる引上げSi結晶は結晶面内の抵抗値のばらつき
が少なく、酸素濃度を制御した高集積回路用ウエ
ハの製造にも使用することができる。
本発明はSi以外の結晶の引上げにも適用するこ
とができる。例えば、GaAsの引上げに適用する
ことによりルツボ材であるシリカやPBN(パイロ
リテイツク窒化ほう素)の溶出を抑制することが
可能である。
According to the present invention, silicon wafers with low oxygen concentrations necessary for power transistors and the like can be manufactured using pulled crystals. In addition, the pulled Si crystal produced by the method of the present invention has little variation in resistance value within the crystal plane, and can be used for manufacturing wafers for highly integrated circuits with controlled oxygen concentration. The present invention can also be applied to pulling crystals other than Si. For example, by applying it to the pulling of GaAs, it is possible to suppress the elution of crucible materials such as silica and PBN (pyrolytic boron nitride).
第1図は本発明の構成を示す模式断面図、第2
図は固/液界面近くの不純物元素濃度分布を示す
模式図、第3図は結晶を回転しない場合の融液流
動を示す模式図、第4図は結晶を回転する場合の
融液流動を示す模式図、第5図は磁場強さと酸素
濃度の関係を示すグラフである。
1……電磁石、2……チエンバ外壁、3……ル
ツボ、4……融液、5……引上げ単結晶、6……
ヒータ、7……熱シールド、10……熱対流、1
1……強制対流。
FIG. 1 is a schematic cross-sectional view showing the configuration of the present invention, and FIG.
The figure is a schematic diagram showing the impurity element concentration distribution near the solid/liquid interface, Figure 3 is a schematic diagram showing the melt flow when the crystal is not rotated, and Figure 4 is a schematic diagram showing the melt flow when the crystal is rotated. The schematic diagram, FIG. 5, is a graph showing the relationship between magnetic field strength and oxygen concentration. 1... Electromagnet, 2... Chamber outer wall, 3... Crucible, 4... Melt, 5... Pulled single crystal, 6...
Heater, 7... Heat shield, 10... Heat convection, 1
1...Forced convection.
Claims (1)
方法において、収容容器内のルツボ側壁近傍の溶
融物質に下向きの進行磁場を印加しながら種結晶
を引上げることにより結晶成長を行うことを特徴
とする単結晶の製造方法。 2 加熱装置を備え溶融物質を収容する単結晶引
上げ用容器と、該容器の側壁の外周を取囲む複数
組のコイルを有する電磁石と、該電磁石のコイル
に各々位相の異なる交流電源を供給する装置とを
設けたことを特徴とする単結晶の製造装置。[Claims] 1. In a method for producing a single crystal from a molten substance by a pulling method, crystal growth is achieved by pulling up a seed crystal while applying a downward traveling magnetic field to the molten substance near the side wall of a crucible in a container. A method for producing a single crystal, characterized by performing the following steps. 2. A single-crystal pulling container equipped with a heating device and containing a molten substance, an electromagnet having multiple sets of coils surrounding the outer periphery of the side wall of the container, and a device for supplying alternating current power with different phases to the coils of the electromagnet. A single-crystal manufacturing device characterized by comprising:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17394085A JPS6236097A (en) | 1985-08-07 | 1985-08-07 | Production of single crystal and device therefor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17394085A JPS6236097A (en) | 1985-08-07 | 1985-08-07 | Production of single crystal and device therefor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6236097A JPS6236097A (en) | 1987-02-17 |
| JPH0351673B2 true JPH0351673B2 (en) | 1991-08-07 |
Family
ID=15969882
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP17394085A Granted JPS6236097A (en) | 1985-08-07 | 1985-08-07 | Production of single crystal and device therefor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6236097A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0362567B1 (en) * | 1988-09-07 | 1992-12-09 | Ishida Scales Mfg. Co., Ltd. | Waterproof automatic weighing apparatus |
| JPH02292428A (en) * | 1989-04-30 | 1990-12-03 | Kudan Kenchiku Kenkyusho:Kk | Cast-in-place-concrete-filled type pc girder |
| JP2013056812A (en) * | 2011-09-09 | 2013-03-28 | Sharp Corp | Method for producing polycrystalline silicon ingot |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6036392A (en) * | 1983-08-05 | 1985-02-25 | Toshiba Corp | Apparatus for pulling single crystal |
-
1985
- 1985-08-07 JP JP17394085A patent/JPS6236097A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6236097A (en) | 1987-02-17 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US5363796A (en) | Apparatus and method of growing single crystal | |
| CA1336061C (en) | High-oxygen-content silicon monocrystal substrate for semiconductor devices and production method therefor | |
| EP0140565B1 (en) | Method for growing multicomponent compound semiconductor crystals | |
| GB2109267A (en) | Processes for solidifying liquid materials | |
| JPH11268987A (en) | Silicon single crystal and its production | |
| JP2688137B2 (en) | Method of pulling silicon single crystal | |
| JP3086850B2 (en) | Method and apparatus for growing single crystal | |
| JPH0212920B2 (en) | ||
| JPS5850953B2 (en) | crystal growth method | |
| US5840116A (en) | Method of growing crystals | |
| JPH0351673B2 (en) | ||
| GB2120954A (en) | Reducing impurity levels in pulled single crystals | |
| JP3750440B2 (en) | Single crystal pulling method | |
| JPS5850951B2 (en) | Crystal growth method and crystal growth equipment used for this method | |
| JPH0524969A (en) | Crystal growth equipment | |
| JPS6236096A (en) | Production of single crystal and device therefor | |
| JPH0480875B2 (en) | ||
| JP3018738B2 (en) | Single crystal manufacturing equipment | |
| JPH09235192A (en) | Low oxygen concentration single crystal ingot and single crystal pulling method | |
| JPS6317291A (en) | Method for growing crystal and device therefor | |
| JP2758038B2 (en) | Single crystal manufacturing equipment | |
| JPH09194284A (en) | Single crystal pulling method | |
| JPS61158897A (en) | Method for pulling up compound semiconductor single crystal and apparatus therefor | |
| JPH0733304B2 (en) | Crystal growth method | |
| JPH0248492A (en) | Single crystal growth apparatus |