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JPS6111915B2 - - Google Patents
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JPS6111915B2 - - Google Patents

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Publication number
JPS6111915B2
JPS6111915B2 JP9610383A JP9610383A JPS6111915B2 JP S6111915 B2 JPS6111915 B2 JP S6111915B2 JP 9610383 A JP9610383 A JP 9610383A JP 9610383 A JP9610383 A JP 9610383A JP S6111915 B2 JPS6111915 B2 JP S6111915B2
Authority
JP
Japan
Prior art keywords
die
shaped silicon
band
spacer
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
Application number
JP9610383A
Other languages
Japanese (ja)
Other versions
JPS59223292A (en
Inventor
Toshuki Sawada
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura Electric Co 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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP9610383A priority Critical patent/JPS59223292A/en
Publication of JPS59223292A publication Critical patent/JPS59223292A/en
Publication of JPS6111915B2 publication Critical patent/JPS6111915B2/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
    • C30B15/00Single-crystal growth by pulling from a melt, e.g. Czochralski method
    • C30B15/34Edge-defined film-fed crystal-growth using dies or slits

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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】[Detailed description of the invention]

〔発明の技術分野〕 本発明は、帯状シリコン結晶製造装置の改良に
関する。 〔発明の技術的背景とその問題点〕 帯状シリコン結晶は薄板状であるため、チヨク
ラルスキー法で得られたインゴツト状のシリコン
結晶とは異なり、その得られた形状のままで半導
体太陽電池の基本として用いられる。従つて、例
えばチヨクラルスキー法で得られるシリコン結晶
を半導体太陽電池の基板として用いるよりも安価
になるという大きな特徴を有する。 帯状シリコン結晶を成長させる炉内の構成の断
面図を第1図に示す。この第1図は、シリコン融
液11を収容する石英ガラス製ルツボ12にカー
ボンで作られたスリツト(間隙)を有するキヤピ
ラリ・ダイ13,13a,13b(以下単にダイ
と言う)をその長辺方向がルツボ12の長辺方向
に平行となるよう設置した状態を示す。ダイ13
の先端部は鋭く、ナイフエツジ状に加工されてお
り、またこれらのダイ13はダイ・ホルダ14,
14a,14bに強く固定されており、さらにダ
イ・ホルダ14は熱遮蔽板15に強く固定されて
いる。熱遮蔽板15はシリコン融液11の熱輻射
が上記ダイ13の先端に到達することを弱める役
割をはたすもので、ダイ13の先端部を露出させ
る窓があけられている。ルツボ12は、カーボン
で形成されたルツボ・ホルダ16内に挿入されて
いる。ルツボ・ホルダ16の外側には、一対の板
状のヒータ17,17a,17bが設けられてい
る。ヒータ17は上記ダイ13およびルツボ・ホ
ルダ16の長手方向に平行に設置され、かつ上下
から交互に切込みが加工されて、これにより電気
抵抗値を制御する仕組みになつている。 上記のように構成された帯状シリコン結晶製造
装置のルツボ12内に多結晶シリコンを入れ、炉
内の温度を約1450〔℃〕に上昇させる。すると、
多結晶シリコンはシリコン融液11となり、この
シリコン融液11が毛細管現象により、ダイ13
の先端部まで上昇する。この上昇したシリコン融
液11に上方から種子結晶(図示せず)を接触さ
せ、種子結晶を徐々に引き上げることにより、帯
状シリコン結晶18を成長させることができる。 しかしながら、この種の装置にあつては、次の
ような問題があつた。すなわち、帯状シリコン結
晶の成長に際しては、ダイ先端の温度分布が極め
て重要であるにも拘わらず、ダイの幅が100
〔mm〕にもなるとダイ先端長手方向に温度差が生
じる。そして、この温度差を3〔℃〕以内に入れ
ることは極めて困難であつた。ダイ先端長手方向
の左右の温度差が3〔℃〕以上になると、ダイの
長手方向両端部に置いた補助温度調節機構等では
十分な調節が不可能となり、バランスよく成長を
行うことはできなくなる。 ダイ先端長手方向温度分布が十分調整された状
態(温度差3℃以内)で成長した帯状シリコン結
晶18とダイ13との関係は第2図に示す如くな
る。しかし、左右の温度分布が調整されていない
と、第3図に示す如く帯状シリコン結晶18が一
方へ片寄つて成長することになる。第3図はダイ
13の左側(図中L側)が右側(図中R側)より
低温であるために、左側の拡幅が大きくなり、右
側が目標地点まで達する前に左端で帯状シリコン
結晶18とダイ13の先端とが固着した例であ
る。この例程温度差が大きくない場合、目標とす
る結晶の幅に到達させることはできる。しかしな
がら、長時間の安定成長を維持することは困難で
あつた。 〔発明の目的〕 本発明の目的は、ダイ先端長手方向の温度分布
を容易かつ確実に一定値以内に制御することがで
き、帯状シリコン結晶の左右の拡幅をバランスよ
く行い得、所望の結晶幅を維持しながら長時間の
安定成長を可能ならしめる帯状シリコン結晶製造
装置を提供することにある。 〔発明の概要〕 本発明の骨子は、ダイ先端部の長手方向左右の
温度差をいかにして小さくし、その再現性を確保
するかと云うことにある。 左右に温度差を発生させている原因は、いくつ
か考えられる。本発明者等はヒータの発熱分布の
差、雰囲気ガスの流れ方の差、熱遮蔽板の材質お
よび加工・組立状況の差等可能性のある部分を検
討したが、いずれが温度差発生の原因であるかを
特定することは困難であつた。しかし、炉内材を
大幅に変更しない限り、一回の成長毎に変換を必
要とするダイ或いは石英ルツボ等を変換しただけ
では、温度分布に再現性があることが判つた。つ
まり、ある炉内構成で左端が低温であつた場合、
その傾向は維持されるということである。また、
本発明者等のさらなる鋭意研究によれば、ダイ先
端長手方向両端部の温度状況を最も容易にかつ確
実に変化させる方法は、ダイ先端部とダイ・ホル
ダ上面との相対位置を変化させることであること
が実験的に判明した。 本発明はこのような点に着目し、ルツボ内に収
容され加熱溶融されたシリコン融液にスリツトを
有するキヤピラリ・ダイの下端を浸漬し、このダ
イのスリツトを介して上昇したシリコン融液に種
子結晶を接触させ、この種結晶を引き上げること
により帯状シリコン結晶を成長形成する帯状シリ
コン結晶製造装置において、前記ダイと該ダイを
固定するダイ・ホルダとの間に所定厚みのスペー
サを配設し、上記ダイの長手方向両端部先端と上
記ホルダの上面との各距離を可変設定するように
したものである。 〔発明の効果〕 本発明によれば、スペーサの厚みを調節するこ
とによりダイの長手方向両端部先端のダイ・ホル
ダ上面からの各距離を可変することができ、これ
によりダイ先端部左右の温度分布を一定範囲内に
容易に調整することができる。しかも、複雑な機
構を付加する必要はないので、操作性が悪くなる
こともない。したがつて、結晶成長時のバランス
良い拡幅を実現でき、より長時間の安定成長が可
能となる。また、本発明者等の実験によれば、帯
状シリコン結晶を所望の幅に拡幅するまでの時間
を従来装置に比して約40〔%〕短縮することが可
能であつた。さらに、左右のスペーサの厚さの差
は最大でも0.4〔mm〕程度で十分であつたので、
これが帯状シリコン結晶の厚さや結晶性等に悪影
響を及ぼすことはなかつた。 〔発明の実施例〕 第4図は本発明の一実施例に係わる帯状シリコ
ン結晶製造装置の概略構成を示す断面図である。
なお、第1図と同一部分には同一符号を付して、
その詳しい説明は省略する。この装置が第1図の
装置と異なる点はキヤピラリ・ダイ、ダイ・ホル
ダの構成及びスペーサを配設したことにある。す
なわち、キヤピラリ・ダイ21,21a,21b
は従来のダイ13と異なり後述するスペーサ2
2,22a,22b,22c22dに密着して、
位置決めの役割を果たすために、長手方向平面上
に1〔mm〕程の段差が設けられている。ダイ・ホ
ルダ23,23a,23bはその内側面に、スペ
ーサ22を収納することができる溝が左右にそれ
ぞれ設けられている。スペーサ22としては、カ
ーボン製のもので、長さ15〔mm〕、幅5〔mm〕、厚
さが約3.5〔mm〕を中心に、0.05〔mm〕刻みに10
種類1種類当り4枚づつ用意した。第5図a〜c
は上記装置の要部構成を部分的に示すもので、第
5図aはダイ・ホルダ23の一片23aにスペー
サ22a,22cが収納された状態の図である。
また、第5図bは、ダイ21aの正面図、第5図
cは、ダイ・ホルダ23に、ダイ21を挾み、ボ
ルトで固定した状態の図である。 ここで問題としているのは、第5図cに示す如
きホルダ上面とダイ先端との距離h1とh2との差
(h1−h2)である。もちろん、ホルダ上面に対して
ダイ先端は、上に出る場合も下に下がる場合もあ
り、h1,h2は前者の場合プラス、後者の場合マイ
ナスとして、その差が重要である。炉内部材を注
意深く構成し、スペーとして厚さ0.35〔mm〕のも
のを4枚共挿入して、ダイ21をダイ・ホルダ2
3に固定して結晶成長を試みた。数回の試行共、
常にダイ21の先端長手方向の左側が右側より7
〜9〔℃〕低いことが判つた。この温度差を0
〔℃〕にすべくh1とh2との差を適当に変化させた
結果を下表に示す。
TECHNICAL FIELD OF THE INVENTION The present invention relates to an improvement in an apparatus for producing band-shaped silicon crystals. [Technical background of the invention and its problems] Because the band-shaped silicon crystal is in the form of a thin plate, unlike the ingot-shaped silicon crystal obtained by the Czyochralski method, it can be used in semiconductor solar cells without changing its shape. Used as a basis. Therefore, it has the great feature that it is cheaper than using, for example, silicon crystal obtained by the Czyochralski method as a substrate for a semiconductor solar cell. FIG. 1 shows a cross-sectional view of the interior of the furnace for growing band-shaped silicon crystals. FIG. 1 shows capillary dies 13, 13a, 13b (hereinafter simply referred to as dies) having slits (gaps) made of carbon in a quartz glass crucible 12 containing a silicon melt 11 in the direction of its long side. The crucible 12 is shown installed so that it is parallel to the long side direction of the crucible 12. die 13
The tips of the dies 13 are sharp and processed into a knife edge shape, and these dies 13 are connected to die holders 14,
14a and 14b, and the die holder 14 is also strongly fixed to a heat shield plate 15. The heat shielding plate 15 serves to weaken the thermal radiation of the silicon melt 11 from reaching the tip of the die 13, and has a window that exposes the tip of the die 13. The crucible 12 is inserted into a crucible holder 16 made of carbon. A pair of plate-shaped heaters 17, 17a, and 17b are provided on the outside of the crucible holder 16. The heater 17 is installed parallel to the longitudinal direction of the die 13 and the crucible holder 16, and cuts are made alternately from above and below, thereby controlling the electrical resistance value. Polycrystalline silicon is placed in the crucible 12 of the belt-shaped silicon crystal manufacturing apparatus constructed as described above, and the temperature inside the furnace is raised to about 1450 [°C]. Then,
Polycrystalline silicon becomes a silicon melt 11, and this silicon melt 11 flows through a die 13 due to capillary action.
rises to the tip of the By bringing a seed crystal (not shown) into contact with the rising silicon melt 11 from above and gradually pulling up the seed crystal, a band-shaped silicon crystal 18 can be grown. However, this type of device has the following problems. In other words, although the temperature distribution at the die tip is extremely important for the growth of band-shaped silicon crystals,
[mm], a temperature difference occurs in the longitudinal direction of the die tip. It was extremely difficult to keep this temperature difference within 3 [°C]. If the temperature difference between the left and right sides in the longitudinal direction of the die tip becomes 3 [℃] or more, sufficient adjustment cannot be made using the auxiliary temperature control mechanisms placed at both longitudinal ends of the die, making it impossible to achieve well-balanced growth. . The relationship between the die 13 and the band-shaped silicon crystal 18 grown in a state where the temperature distribution in the longitudinal direction of the die tip is sufficiently adjusted (temperature difference within 3° C.) is as shown in FIG. However, if the left and right temperature distribution is not adjusted, the band-shaped silicon crystal 18 will grow biased to one side, as shown in FIG. In FIG. 3, since the left side (L side in the figure) of the die 13 is lower temperature than the right side (R side in the figure), the width of the left side increases, and the band-shaped silicon crystal 18 reaches the left end before the right side reaches the target point. This is an example in which the tip of the die 13 and the tip of the die 13 are stuck together. If the temperature difference is not as large as in this example, it is possible to reach the target crystal width. However, it has been difficult to maintain stable growth over a long period of time. [Object of the Invention] An object of the present invention is to be able to easily and reliably control the temperature distribution in the longitudinal direction of the die tip within a certain value, to widen the band-shaped silicon crystal from side to side in a well-balanced manner, and to obtain the desired crystal width. An object of the present invention is to provide an apparatus for producing band-shaped silicon crystals that enables stable growth over a long period of time while maintaining the following properties. [Summary of the Invention] The gist of the present invention is how to reduce the temperature difference between the left and right sides of the die tip in the longitudinal direction and ensure its reproducibility. There are several possible causes of the temperature difference between the left and right sides. The inventors investigated possible factors such as differences in the heat generation distribution of the heaters, differences in the flow of atmospheric gas, and differences in the material and processing/assembly conditions of the heat shield plate, but which of the following could be the cause of the temperature difference? It was difficult to determine whether the However, it has been found that the temperature distribution is reproducible only by changing the die, quartz crucible, etc., which require conversion for each growth, as long as the furnace interior materials are not significantly changed. In other words, if the left end is at a low temperature in a certain furnace configuration,
That trend is expected to be maintained. Also,
According to further intensive research by the present inventors, the easiest and most reliable way to change the temperature situation at both longitudinal ends of the die tip is to change the relative position between the die tip and the top surface of the die holder. It has been experimentally discovered that. The present invention focuses on such points, and the lower end of a capillary die with a slit is immersed in a heated and melted silicon melt housed in a crucible, and seeds are injected into the silicon melt rising through the slit of the die. In a band-shaped silicon crystal manufacturing apparatus that grows and forms a band-shaped silicon crystal by bringing crystals into contact with each other and pulling up the seed crystal, a spacer of a predetermined thickness is disposed between the die and a die holder that fixes the die, Each distance between the tips of both longitudinal ends of the die and the top surface of the holder is variably set. [Effects of the Invention] According to the present invention, by adjusting the thickness of the spacer, it is possible to vary the distances of the tips of both longitudinal ends of the die from the top surface of the die holder. The distribution can be easily adjusted within a certain range. Furthermore, since there is no need to add a complicated mechanism, operability will not deteriorate. Therefore, it is possible to achieve well-balanced widening during crystal growth, and stable growth for a longer period of time is possible. Furthermore, according to experiments conducted by the present inventors, it was possible to reduce the time required to widen a band-shaped silicon crystal to a desired width by about 40% compared to the conventional apparatus. Furthermore, the maximum difference in thickness between the left and right spacers was about 0.4 mm, so
This did not have any adverse effect on the thickness, crystallinity, etc. of the band-shaped silicon crystal. [Embodiment of the Invention] FIG. 4 is a sectional view showing a schematic configuration of a belt-shaped silicon crystal manufacturing apparatus according to an embodiment of the present invention.
The same parts as in Fig. 1 are given the same reference numerals.
A detailed explanation thereof will be omitted. This device differs from the device shown in FIG. 1 in the configuration of the capillary die and die holder, and the arrangement of spacers. That is, the capillary dies 21, 21a, 21b
is different from the conventional die 13 and has a spacer 2 which will be described later.
2, 22a, 22b, 22c and 22d,
In order to play the role of positioning, a step of about 1 mm is provided on the longitudinal plane. The die holders 23, 23a, and 23b are provided with grooves on the left and right sides thereof, respectively, in which the spacers 22 can be accommodated. The spacer 22 is made of carbon and has a length of 15 [mm], a width of 5 [mm], and a thickness of about 3.5 [mm], with 10 increments of 0.05 [mm].
Four sheets were prepared for each type. Figure 5 a-c
5 partially shows the configuration of the main parts of the device, and FIG. 5a shows a state in which spacers 22a and 22c are housed in one piece 23a of the die holder 23.
5b is a front view of the die 21a, and FIG. 5c is a diagram showing the die 21 held in the die holder 23 and fixed with bolts. What is at issue here is the difference (h 1 -h 2 ) between the distances h 1 and h 2 between the top surface of the holder and the tip of the die as shown in FIG. 5c. Of course, the die tip may protrude upward or downward relative to the upper surface of the holder, and the difference between h 1 and h 2 is important, as they are positive in the former case and negative in the latter case. Carefully configure the furnace interior materials, insert four pieces of 0.35 mm thick spacers, and place the die 21 into the die holder 2.
3 and tried crystal growth. After several attempts,
The left side of the tip of the die 21 in the longitudinal direction is always 7
It was found that the temperature was ~9 [°C] lower. This temperature difference is 0
The table below shows the results of appropriately changing the difference between h 1 and h 2 to achieve [°C].

【表】 この表に示したように、高さの差が0.30〔mm〕
になるように、スペーサ厚を左側の2個は3.45
〔mm〕、右側の2個は、3.75〔mm〕とした。これら
のスペーサを同様に挿入した数回の実験で、所望
の温度差3〔℃〕以内を常に維持することが可能
であつた。また、炉内材を大幅に変換した場合、
左右の温度分布が逆転することもあつたが、温度
差が9〔℃〕を超えることはなかつた。そして、
高さの差も0.40〔mm〕を超えて補正する必要はな
かつた。 ダイ上端の左側が右側よりも7〜9〔℃〕低い
場合、帯状シリコン結晶は左側へのみ拡幅して行
き、右側へは殆んど拡幅しなかつた。結晶が左端
に到達してしまつても、右側へは拡幅が不十分な
ため、所望とする幅100〔mm〕には到らなかつ
た。ダイ上端左側が3〜5〔℃〕低い程度に高さ
を補正して成長を試みた。高さの差は、0.20
〔mm〕であつた。この場合も結晶が左側へ大きく
拡幅したので、ダイ中央部から左側へ片寄つた位
置で成長しながら、補助温度調節機構の助けを借
りてどうにか幅100〔mm〕に到つた。しかしなが
ら、全面的には左側の方が低温であり、ダイ先端
部と固液界面との距離は右側より左側の方が小さ
く不安定であつたため、幅100〔mm〕の状態を長
時間続けることは困難であつた。 一方、高さの差を0.30〔mm〕として、左右の温
度差を略0〔℃〕として、成長を行つたところ、
左右への拡幅はバランス良く行われ、補助温度調
節装置を拡幅のために使う必要はなかつた。この
ように無理なく拡幅が行なわれたために、目的の
幅100〔mm〕に達するまでの時間も、温度差約3
〔℃〕の時よりも40〔%〕も短い時間であつた。
また、幅100〔mm〕に達してから、この幅を維持
しながらの制御も容易であり、ルツボ内融液がな
くなるまで安定に成長を続けることができた。そ
の後実験を繰り返して行つたが、前回の成長実験
の温度分布を参考に、高さ(h1,h2)の補正を行
うことによつて、ダイ上端左右の温度差を常に2
〔℃〕以内に入れることは容易であつた。また、
ダイ上端長手方向の温度分布の均一化により、結
晶の厚みも一定となつた。温度の低い部分は固液
界面が低くなりそれに伴つて結晶の厚みも増して
くるが、温度分布を補正することによつて帯状シ
リコン結晶の一端が厚い傾向も補正されて、両端
の厚さは略同一になつた。厚さが一定になること
は太陽電池化の際の電極形成歩留りの向上に寄与
する。 以上説明した実施例から明らかなように、ダイ
先端のダイ・ホルダ上面からの突出程度を加減す
るために、ダイ・ホルダとダイとの間にスペーサ
を挿入することにより、ダイ先端長手方向左右間
の温度分布を容易かつ確実に補正することがで
き、帯状シリコン結晶の拡幅時間を短縮すること
ができた。その上、ダイ左右間の温度バランスが
良好なために、無理なく一定の結晶幅を維持する
ことが可能となり、その結果長時間の安定成長が
実現した。帯状シリコン結晶の低コスト化とし
て、成長速度を上げること、幅を大きくするこ
と、途中で成長が中断しないこと等が主な狙い目
であるが、本発明によつて少くとも後二者が実現
され、太陽電池の低コスト化に大きく寄与するも
のである。 なお、本発明は上述した実施例に限定されるも
のではない。実施例ではダイ・ホルダ上面とダイ
先端との高さは略等しい構成となつていたが、ダ
イ・ホルダ上面にダイの先端部と同じ高さになる
ように加工或いは組合されたカーボン板等を設置
することがある。この場合、上記カーボン等に対
してダイ先端長手方向の高さを変えるべくダイを
傾けても前述したのと同様な効果が得られた。ま
た、ダイ・ホルダとダイとの間にスペーサを入れ
たがスペーサの枚数は4枚に限定されるものでは
なく、その材質もカーボンに限らない。スペーサ
の材質としては、耐熱、耐シリコン蒸気に優れ、
有害不純物の含有量が少く加工性の良いものであ
ればよい。 また、スペーサは、必ずしもダイ・ホルダ或い
はダイに固定させる必要はない。さらに、スペー
サにテーパを設け成長炉外に出した操作治具によ
りこのスペーサをダイに対して動かし、これによ
りダイの高さをスペーサのテーパに従つて変化さ
せることも可能である。その他、本発明の要旨を
逸脱しない範囲で種々変形して実施することがで
きる。
[Table] As shown in this table, the height difference is 0.30 [mm]
The spacer thickness for the two on the left is 3.45 so that
[mm], and the two on the right were 3.75 [mm]. In several experiments in which these spacers were inserted in the same way, it was possible to always maintain the desired temperature difference within 3 [° C.]. In addition, if the furnace interior material is significantly changed,
Although the temperature distribution between the left and right sides was sometimes reversed, the temperature difference never exceeded 9 [°C]. and,
There was no need to correct the height difference by more than 0.40 [mm]. When the left side of the top of the die was 7 to 9 degrees Celsius lower than the right side, the band-shaped silicon crystal expanded only to the left, and hardly expanded to the right. Even when the crystal reached the left end, the desired width of 100 [mm] could not be reached because the width was insufficiently widened to the right. Growth was attempted by correcting the height so that the left side of the upper end of the die was 3 to 5 degrees Celsius lower. The difference in height is 0.20
It was [mm]. In this case as well, the crystal widened significantly to the left, so it grew to the left from the center of the die and somehow reached a width of 100 mm with the help of an auxiliary temperature control mechanism. However, overall the temperature was lower on the left side, and the distance between the die tip and the solid-liquid interface was smaller and unstable on the left side than on the right side, so it was difficult to maintain the width of 100 mm for a long time. was difficult. On the other hand, when growth was performed with a height difference of 0.30 [mm] and a temperature difference between the left and right sides of approximately 0 [℃],
The width expansion from left to right was well balanced, and there was no need to use an auxiliary temperature control device for width expansion. Because the width was expanded without much effort, the time it took to reach the desired width of 100 mm was also shortened by a temperature difference of about 3 mm.
The time was 40% shorter than at [℃].
Furthermore, once the width reached 100 mm, it was easy to maintain this width and continue to grow stably until the melt in the crucible ran out. After that, the experiment was repeated, but by correcting the height (h 1 , h 2 ) with reference to the temperature distribution of the previous growth experiment, the temperature difference between the left and right sides of the top of the die was always kept at 2.
It was easy to keep the temperature within [°C]. Also,
By making the temperature distribution uniform in the longitudinal direction of the upper end of the die, the thickness of the crystal also became constant. In areas with low temperatures, the solid-liquid interface becomes lower and the crystal thickness increases accordingly, but by correcting the temperature distribution, the tendency for one end of the band-shaped silicon crystal to be thick is also corrected, and the thickness at both ends becomes became almost the same. Having a constant thickness contributes to improving the electrode formation yield during solar cell production. As is clear from the embodiments described above, in order to adjust the degree of protrusion of the die tip from the upper surface of the die holder, by inserting a spacer between the die holder and the die, the distance between the left and right sides in the longitudinal direction of the die tip can be adjusted. temperature distribution could be easily and reliably corrected, and the time required to widen the band-shaped silicon crystal could be shortened. Furthermore, since the temperature balance between the left and right sides of the die is good, it is possible to maintain a constant crystal width without difficulty, and as a result, stable growth over a long period of time has been achieved. In order to reduce the cost of band-shaped silicon crystals, the main aims are to increase the growth rate, increase the width, and prevent growth from being interrupted midway, and the present invention achieves at least the latter two. This will greatly contribute to lowering the cost of solar cells. Note that the present invention is not limited to the embodiments described above. In the example, the heights of the top surface of the die holder and the tip of the die were approximately equal; It may be installed. In this case, even if the die was tilted to change the height in the longitudinal direction of the die tip relative to the carbon, etc., the same effect as described above was obtained. Further, although a spacer is inserted between the die holder and the die, the number of spacers is not limited to four, and the material of the spacer is not limited to carbon. The material of the spacer has excellent heat resistance and silicon vapor resistance.
Any material with low content of harmful impurities and good processability may be used. Also, the spacer does not necessarily need to be fixed to the die holder or die. Furthermore, it is also possible to provide a spacer with a taper and move this spacer relative to the die using an operating jig taken out of the growth furnace, thereby changing the height of the die in accordance with the taper of the spacer. In addition, various modifications can be made without departing from the gist of the present invention.

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

第1図は従来の帯状シリコン結晶製造装置の概
略構成を示す断面図、第2図及び第3図はそれぞ
れ上記従来装置の問題点を説明するための模式
図、第4図は本発明の一実施例の概略構成を示す
断面図、第5図a〜cはそれぞれ上記実施例の要
部構成を部分的に示す図である。 11……シリコン融液、12……ルツボ、15
……熱遮蔽板、17,17a,17b……ヒー
タ、18……帯状シリコン結晶、21,21a,
21b……キヤピラリ・ダイ、22,22a〜2
2d……スペーサ、23,23a,23b……ダ
イ・ホルダ。
FIG. 1 is a cross-sectional view showing a schematic configuration of a conventional belt-shaped silicon crystal production apparatus, FIGS. 2 and 3 are schematic diagrams for explaining the problems of the conventional apparatus, and FIG. 5A to 5C are cross-sectional views showing the schematic structure of the embodiment, and FIGS. 5A to 5C are views partially showing the main structure of the above embodiment. 11... Silicon melt, 12... Crucible, 15
... Heat shield plate, 17, 17a, 17b ... Heater, 18 ... Band-shaped silicon crystal, 21, 21a,
21b...Capillary die, 22, 22a-2
2d...Spacer, 23, 23a, 23b...Die holder.

Claims (1)

【特許請求の範囲】 1 ルツボ内に収容され加熱溶融されたシリコン
融液にスリツトを有するキヤピラリ・ダイの下端
を浸漬し、このダイのスリツトを介して上昇した
シリコン融液に種子結晶を接触させ、この種子結
晶を引き上げることにより帯状シリコン結晶を成
長形成する帯状シリコン結晶製造装置において、
前記ダイ該ダイを固定するダイ・ホルダとの間に
所定厚みのスペーサを配設し、上記ダイの長手方
向両端部先端と上記ホルダの上面との各距離を可
変設定してなることを特徴とする帯状シリコン結
晶製造装置。 2 前記スペーサは、カーボンからなるものであ
ることを特徴とする特許請求の範囲第1項記載の
の帯状シリコン結晶製造装置。
[Claims] 1. The lower end of a capillary die having a slit is immersed in a heated and melted silicon melt housed in a crucible, and a seed crystal is brought into contact with the silicon melt rising through the slit of the die. In a band-shaped silicon crystal manufacturing apparatus that grows and forms band-shaped silicon crystals by pulling up this seed crystal,
A spacer having a predetermined thickness is disposed between the die and a die holder that fixes the die, and distances between the ends of both longitudinal ends of the die and the top surface of the holder are variably set. Band-shaped silicon crystal manufacturing equipment. 2. The belt-shaped silicon crystal manufacturing apparatus according to claim 1, wherein the spacer is made of carbon.
JP9610383A 1983-05-31 1983-05-31 Device for producing belt-like silicon crystal Granted JPS59223292A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9610383A JPS59223292A (en) 1983-05-31 1983-05-31 Device for producing belt-like silicon crystal

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9610383A JPS59223292A (en) 1983-05-31 1983-05-31 Device for producing belt-like silicon crystal

Publications (2)

Publication Number Publication Date
JPS59223292A JPS59223292A (en) 1984-12-15
JPS6111915B2 true JPS6111915B2 (en) 1986-04-05

Family

ID=14156048

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9610383A Granted JPS59223292A (en) 1983-05-31 1983-05-31 Device for producing belt-like silicon crystal

Country Status (1)

Country Link
JP (1) JPS59223292A (en)

Also Published As

Publication number Publication date
JPS59223292A (en) 1984-12-15

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