JPH0840717A - Fluidized bed reactor for monosilane decomposition - Google Patents
Fluidized bed reactor for monosilane decompositionInfo
- Publication number
- JPH0840717A JPH0840717A JP17648094A JP17648094A JPH0840717A JP H0840717 A JPH0840717 A JP H0840717A JP 17648094 A JP17648094 A JP 17648094A JP 17648094 A JP17648094 A JP 17648094A JP H0840717 A JPH0840717 A JP H0840717A
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- Japan
- Prior art keywords
- gas
- reactor
- silicon
- particles
- wall
- 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.)
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- Silicon Compounds (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、モノシランの熱分解に
より多結晶シリコンを製造するためのモノシラン分解用
流動床反応器に関するものである。FIELD OF THE INVENTION The present invention relates to a fluidized bed reactor for monosilane decomposition for producing polycrystalline silicon by thermal decomposition of monosilane.
【0002】[0002]
【従来の技術】従来、多結晶シリコンは、モノシラン
(シラン)の熱分解反応により、シリコン棒上に析出し
て製造されている。この製造方法では、ベルジャーと称
する反応炉が用いられ、反応炉の壁面にシリコンが析出
するのを防止するために炉壁を冷却しており、熱効率が
悪い欠点がある。しかも、この方法では、析出面積が小
さいため、シリコンの析出速度が遅いこと、またバッチ
式であるために生産性が悪いという不利がある。かかる
技術の欠点を克服するため、流動化した実質的に析出面
積の大きな細かいシリコン顆粒上にシリコンを析出させ
る方法(流動化多結晶シリコン製造方法)が提案され
た。2. Description of the Related Art Conventionally, polycrystalline silicon has been manufactured by depositing it on a silicon rod by a thermal decomposition reaction of monosilane (silane). In this manufacturing method, a reaction furnace called a bell jar is used, and the furnace wall is cooled in order to prevent silicon from precipitating on the wall surface of the reaction furnace. In addition, this method has the disadvantages that the deposition area is small and thus the deposition rate of silicon is slow, and that the productivity is poor because it is a batch system. In order to overcome the drawbacks of this technique, a method (fluidized polycrystalline silicon production method) of depositing silicon on fluidized fine silicon granules having a substantially large deposition area has been proposed.
【0003】特開昭58−204814号公報には、反
応管の直径を場所によって変えた流動床式反応器を用
い、反応管内を下から上へ流れるモノハロシランを含有
するガスの流量を変えて、高純度シリコン顆粒上にシリ
コンを析出させつつ、流動床内に浮遊するシリコン顆粒
の大きさの範囲を広くする多結晶シリコン粒子の製造方
法が開示されている。In Japanese Patent Laid-Open No. 58-204814, a fluidized bed reactor in which the diameter of the reaction tube is changed depending on the location is used and the flow rate of the gas containing monohalosilane flowing from the bottom to the top in the reaction tube is changed. A method for producing polycrystalline silicon particles is disclosed, in which silicon is deposited on high-purity silicon granules and the size range of the silicon granules floating in a fluidized bed is widened.
【0004】また、特開昭57−145021号公報に
は、上開きのテーパーを持つ流動床反応器内に底部にあ
る複数のノズルからクロロシランと水素ガスを導入して
反応器内にシリコン微粒子を流動させかつ該微粒子にシ
リコンを析出させ顆粒状に成長した多結晶シリコン粒子
を製造する方法が開示されている。上記の方法はいずれ
もモノハロシランあるいはモノクロルシランを原料とす
る多結晶シリコン粒子の製造法である。他方、加熱流動
床反応器において、モノシランの熱分解による多結晶シ
リコン粒子の製造法も知られている。ところが、従来の
モノシランの熱分解による多結晶シリコンの製造に使用
する加熱流動床反応器においては、反応器直径及び使用
粒子径によっては、流動化したシリコン粒子が凝結して
反応器内で閉鎖したり、流動床で形成される分解用ガス
(シランと水素)の泡が反応器直径以上の大きさとなっ
てスラッグフローとなり、高シラン変換率が得られない
というハロシランを原料とする製造方法では起こらない
問題があった。Further, in Japanese Patent Application Laid-Open No. 57-145021, chlorosilane and hydrogen gas are introduced from a plurality of nozzles at the bottom into a fluidized bed reactor having a taper opening upward so that silicon microparticles are introduced into the reactor. Disclosed is a method of producing granular polycrystalline silicon particles by flowing and depositing silicon on the particles. The above methods are all methods for producing polycrystalline silicon particles using monohalosilane or monochlorosilane as a raw material. On the other hand, a method for producing polycrystalline silicon particles by thermal decomposition of monosilane in a heating fluidized bed reactor is also known. However, in the conventional heating fluidized bed reactor used for producing polycrystalline silicon by thermal decomposition of monosilane, depending on the reactor diameter and the particle size used, fluidized silicon particles are condensed and closed in the reactor. Or, the bubbles of the decomposition gas (silane and hydrogen) formed in the fluidized bed become larger than the reactor diameter and become slug flow, which does not occur in the production method using halosilane as a raw material that a high silane conversion rate cannot be obtained. There was no problem.
【0005】[0005]
【発明が解決しようとする課題】流動化したシリコン顆
粒上にモノシランの熱分解により生成したシリコンを析
出させる方法でのガス線速は通常 2×Umf≦U≦8
×Umf (U:ガス線速、Umf:使用粒子の最小流
動化速度)が好ましいことが知れている。その理由はU
≦2×Umf の場合、シリコンが凝結し、8×Umf
≦Uの場合、流動床で形成されるガスの泡が反応器直径
以上の大きさとなってスラッグフローとなって、高いシ
ランの変換率が得られないためである。反応器直径及び
使用粒子径によっては、この範囲のガス線速でも、シリ
コンが凝結したり、流動床で形成される分解用ガス(シ
ランと水素)の泡が反応器直径以上の大きさとなってス
ラッグフローとなる。通常の円筒状反応器で1000μ
mのシリコン粒子を用いて流動化多結晶シリコン製造を
行う場合、ガス線速がU=6×Umfでも流動床で形成
されるガスの泡の径が200mmにも達し、反応器直径
が200mm未満では流動床全体がスラッグフローとな
り、高いシランの変換率が得れないという問題があっ
た。またコーン状の反応器を用いた流動化多結晶シリコ
ン製造方法もいくつか提案されているが、いずれも、出
発材料としての250〜500μmの微粒子から1〜2
mmの顆粒に至る幅広い粒度分布を持つシリコン粒子を
良好な流動状態に保持することを目的としているため
に、コーンの角度が広すぎて該粒度分布を持つシリコン
粒子を用いて、原料ガス中のモノシラン濃度を10mo
l%で行う場合、ガス線速がU=6×Umfでも流動床
上部のガス線速度が小さくなった部分でシリコン粒子の
凝結が起こり反応の継続ができないという問題があっ
た。The gas linear velocity in the method of depositing silicon produced by thermal decomposition of monosilane on fluidized silicon granules is usually 2 × Umf ≦ U ≦ 8.
It is known that × Umf (U: gas linear velocity, Umf: minimum fluidization velocity of used particles) is preferable. The reason is U
When ≦ 2 × Umf, silicon is condensed and 8 × Umf
This is because when ≦ U, the gas bubbles formed in the fluidized bed have a size larger than the reactor diameter and become slug flow, and a high conversion rate of silane cannot be obtained. Depending on the reactor diameter and the particle size used, even at a gas linear velocity in this range, silicon condenses and bubbles of the decomposition gas (silane and hydrogen) formed in the fluidized bed become larger than the reactor diameter. It will be a slug flow. 1000μ in a normal cylindrical reactor
When fluidized polycrystalline silicon is produced by using m silicon particles, the diameter of gas bubbles formed in the fluidized bed reaches 200 mm even if the gas linear velocity is U = 6 × Umf, and the reactor diameter is less than 200 mm. However, there was a problem that the entire fluidized bed became slug flow and a high conversion rate of silane could not be obtained. Further, some methods for producing fluidized polycrystalline silicon using a cone-shaped reactor have been proposed.
Since the purpose is to keep the silicon particles having a wide particle size distribution up to granules of mm in a good flow state, the cone angle is too wide and the silicon particles having the particle size distribution are used to Monosilane concentration of 10mo
When it was carried out at 1%, there was a problem that even if the gas linear velocity was U = 6 × Umf, the silicon particles were condensed at the portion where the gas linear velocity in the upper part of the fluidized bed became small and the reaction could not be continued.
【0006】[0006]
【課題を解決するための手段】本発明の目的は、これら
の問題点すべてを解決して、シリコン粒子の凝結を抑え
ると共に、高いシラン変換率を達成し得るモノシラン分
解用流動床反応器を提供することにある。本発明の他の
目的は、モノシランの熱分解による多結晶シリコンの製
造に使用する加熱流動床反応器に特定の形状を選択して
シリコン粒子の凝結を抑え、かつ高シラン変換率を達成
し得るモノシラン分解用流動床反応器を提供することに
ある。The object of the present invention is to provide a fluidized bed reactor for monosilane decomposition capable of solving all of these problems, suppressing the condensation of silicon particles, and achieving a high silane conversion rate. To do. Another object of the present invention is to select a specific shape for the heated fluidized bed reactor used for the production of polycrystalline silicon by the thermal decomposition of monosilane to suppress the condensation of silicon particles and to achieve a high silane conversion rate. It is to provide a fluidized bed reactor for decomposing monosilane.
【0007】本発明のさらに他の目的および利点は以下
の説明から明らかになろう。本発明によれば、本発明の
上記目的および利点は、上開きの錐体を形成する壁を有
しそしてこの壁が鉛直線となす角度が1.3〜3.9゜の
範囲にあることを特徴とするモノシラン分解流動床反応
器によって達成される。Further objects and advantages of the present invention will be apparent from the following description. According to the present invention, the above objects and advantages of the present invention are to have a wall forming an upwardly-opening cone and the angle between this wall and the vertical being in the range of 1.3 to 3.9 °. Is achieved by a monosilane decomposition fluidized bed reactor.
【0008】流動化したシリコン顆粒上にシリコンを析
出させる方法でのガス線速は、通常2≦U/Umf≦8
(U:ガス線速、Umf:使用粒子の最小流動化速
度)が好ましいことが知られているが、本発明者等はシ
リコン粒子の凝結のしやすさは分解用ガス中のシラン濃
度とガス線速の相関に支配されると考えて、シリコンの
凝結を起こす場合の分解用ガス中のシラン濃度とガス線
速との関係について調査した。図1は、シリコン粒子が
凝結を起こす場合と起こさない場合の分解用ガス中のシ
ラン濃度とガス線速との関係である。図1中の実験デー
タは、反応温度、シラン濃度、流動層高さ、粒子径等も
様々である。この図1から、シリコンが凝結を起こさな
いためには、分解用ガス中のシラン濃度が高い場合に
は、大きなガス線速を必要とするが、分解用ガス中のシ
ラン濃度が低い場合には、小さなガス線速でもシリコン
の凝結が起きないことが見出された。そして分解用ガス
が下から上に流れる間に分解用ガス中のシランがシリコ
ンに変換し、シラン濃度が低下することに着目して、分
解用ガスが下から上に流れる間のシラン濃度の低下に併
せてガス線速を前記凝結を起こさない限度で小さくでき
ること、即ち、反応器直径を大きくすることができるこ
とを見出した。このように反応器直径を下から上に向か
うにつれて大きくしていくことによって流動床で形成さ
れるガスの泡が仮に一旦、反応直径以上の大きさとなっ
てスラッグフローとなっても泡が下から上に向かうにつ
れて反応器直径に比して小さくなる結果となってスラッ
グフローが解消され、シリコン粒子と分解用ガスとの接
触効率がよくなりシラン変換率を向上させ、かつシリコ
ンの凝結も起さないというような反応器形状が存在する
ことを見出した。The gas linear velocity in the method of depositing silicon on fluidized silicon granules is usually 2≤U / Umf≤8.
It is known that (U: linear velocity of gas, Umf: minimum fluidization velocity of particles used) is preferable, but the present inventors have found that the easiness of condensation of silicon particles depends on the silane concentration in the decomposition gas and the gas. The relationship between the linear velocity of gas and the silane concentration in the decomposition gas when silicon is condensed was investigated, considering that it is governed by the correlation of linear velocity. FIG. 1 shows the relationship between the silane concentration in the decomposition gas and the linear gas velocity when the silicon particles cause condensation and when they do not. The experimental data in FIG. 1 has various reaction temperatures, silane concentrations, fluidized bed heights, particle diameters, and the like. From FIG. 1, in order to prevent silicon from condensing, a large gas linear velocity is required when the silane concentration in the decomposition gas is high, but when the silane concentration in the decomposition gas is low. , It was found that silicon condensation does not occur even at a small gas linear velocity. While the decomposition gas flows from the bottom to the top, the silane in the decomposition gas is converted into silicon, and the silane concentration decreases, paying attention to the decrease in the silane concentration while the decomposition gas flows from the bottom to the top. In addition, it was found that the gas linear velocity can be reduced within the limit that does not cause the condensation, that is, the reactor diameter can be increased. In this way, by increasing the reactor diameter from the bottom to the top, the bubbles of gas formed in the fluidized bed temporarily become larger than the reaction diameter, and even if the slug flow occurs, the bubbles will rise from the bottom. As it goes up, it becomes smaller than the reactor diameter, the slug flow is eliminated, the contact efficiency between the silicon particles and the decomposition gas is improved, the silane conversion rate is improved, and the condensation of silicon also occurs. It was found that there is a reactor shape that does not exist.
【0009】上開きの錐体を形成する壁を有し、該壁と
鉛直線とのなす角度が0゜(即ち、直銅型)、または
1.3゜より小さいと、1000μmのシリコン粒子を
用いて、ガス線速がU=6×Umfで行う場合、流動床
で形成されるガスの泡が反応器直径以上の大きさとなっ
てスラッグフローとなり、泡が下から上に向かっても反
応器直径より小さくならないためにスラッグフローが解
消されず、モノシランの高い変換率は得られない。If there is a wall forming an upwardly-opened cone and the angle between the wall and the vertical line is 0 ° (that is, straight copper type) or less than 1.3 °, silicon particles of 1000 μm are generated. When using a linear gas velocity of U = 6 × Umf, the gas bubbles formed in the fluidized bed become slug flow with a size larger than the reactor diameter, and the bubbles flow from bottom to top in the reactor. Since the diameter is not smaller than the diameter, the slug flow is not eliminated, and the high conversion rate of monosilane cannot be obtained.
【0010】一方、上開きの錐体よりなる壁を有し、該
壁と鉛直線とのなす角度が3.9゜より大きいと250
〜500μmの微粒子から1〜2mmの顆粒に至る幅広
い粒度分布を持つシリコン粒子を用いて原料ガス中のモ
ノシラン濃度を10mol%で行う場合、ガス線速がU
=6×Umfでも流動床上部でのガス線速が小さくなり
シリコンの凝結が起こる。On the other hand, it has a wall made of an upwardly-opening cone, and if the angle between the wall and the vertical line is larger than 3.9 °, it is 250.
When the monosilane concentration in the source gas is 10 mol% using silicon particles having a wide particle size distribution ranging from fine particles of up to 500 μm to granules of 1 to 2 mm, the linear gas velocity is U.
= 6 × Umf, the gas linear velocity in the upper part of the fluidized bed becomes small and silicon condenses.
【0011】次に、この発明の詳細な図面に基づいて説
明する。図2は、この発明の一実施例における反応容器
1の断面図であり、上開きの錐体を形成する壁を有し、
該壁と鉛直線とのなす角度が3.0゜である。反応容器
1は底部の直径200mm、上部の直径が514mm
で、上部にガス抜き管7と、シリコンの種粒子を容器内
に挿入するための供給管3とを備えている。反応容器1
の底部には、原料モノシランガス導入管4と水素ガス導
入管5とできた顆粒状シリコンの抜出管6が設けてあ
る。顆粒状シリコンの抜出管6はガス分散板8の中心部
に設けてある。また、ガス分散板8より上方には、反応
容器1を包囲するようにヒータ2が設けてある。ガス抜
き管7にはガスサンプリング口9が設けてある。反応容
器1内に多結晶シリコンからなり250〜500μmの
微粒子から1000μmの顆粒に至る幅広い粒度分布を
持つ種粒子を静止層高が1000mmとなるように充填
し、容器内をヒータ2で加熱しながら原料ガス導入管4
及び水素導入管5よりモノシラン濃度が10mol%、
ガス線速がU=6×Umfとなるように反応容器1内に
ガスを吹き込む。反応容器1内に吹き込まれたガスは反
応容器1内を上昇し、この過程で物理的には容器内のシ
リコン粒子を流動化させて流動層を形成し、化学的には
流動層を形成するシリコン粒子の表面にシリコンを析出
させて、シリコン粒子を成長させる。この間、遂次ガス
サンプリング口9よりガス中のモノシラン濃度をオンラ
インでガスクロマトグラフ10により測定する。所定の
析出反応を終えたシリコンは、顆粒状シリコンの抜出管
6より反応容器1外に遂次抜き出され、代わりに供給管
3からは種粒子が反応容器内へ挿入される。シリコン析
出反応に使用された後のガスは、ガス抜き管7より反応
容器1外に排出される。Next, a detailed description of the present invention will be given with reference to the drawings. FIG. 2 is a cross-sectional view of the reaction container 1 according to one embodiment of the present invention, which has a wall forming a cone that opens upward,
The angle between the wall and the vertical line is 3.0 °. The reaction vessel 1 has a bottom diameter of 200 mm and an upper diameter of 514 mm.
The upper part is provided with a gas vent pipe 7 and a supply pipe 3 for inserting silicon seed particles into the container. Reaction vessel 1
At the bottom of the column, there is provided a raw material monosilane gas introduction pipe 4 and a hydrogen gas introduction pipe 5 for extracting granular silicon 6 made of granular silicon. The extraction tube 6 for granular silicon is provided at the center of the gas dispersion plate 8. A heater 2 is provided above the gas dispersion plate 8 so as to surround the reaction container 1. The gas vent pipe 7 is provided with a gas sampling port 9. The reaction vessel 1 was filled with seed particles made of polycrystalline silicon and having a wide particle size distribution from 250 to 500 μm fine particles to 1000 μm granules so that the static bed height was 1000 mm, and the inside of the vessel was heated by the heater 2. Raw material gas introduction pipe 4
And the concentration of monosilane from the hydrogen introducing pipe 5 is 10 mol%,
Gas is blown into the reaction vessel 1 so that the gas linear velocity is U = 6 × Umf. The gas blown into the reaction vessel 1 rises in the reaction vessel 1, and in this process physically fluidizes the silicon particles in the vessel to form a fluidized bed, and chemically forms a fluidized bed. Silicon is deposited on the surface of the silicon particles to grow the silicon particles. During this period, the concentration of monosilane in the gas is measured online from the successive gas sampling port 9 by the gas chromatograph 10. The silicon that has undergone the predetermined deposition reaction is sequentially withdrawn from the reaction container 1 through the granular silicon withdrawal pipe 6, and seed particles are inserted into the reaction container from the supply pipe 3 instead. The gas used for the silicon deposition reaction is discharged from the reaction vessel 1 through the gas vent pipe 7.
【0012】[0012]
【作用】本発明の反応器においては、流動床で形成され
る分解用ガス(シランと水素)の泡が反応容器直径以上
の大きさとなっても泡が上昇するにつれて反応器直径が
大きくなるので所定の高さ以上では、泡が反応器直径以
下となり、スラッグフローが解消され、シランの高い変
換率が得られる。また、流動床上部でのガス線速は2×
Umf≦Uとなるのでガス線速の低下によるシリコン粒
子の凝結も起こらない。反応器の形状は、上開きの錐体
を形成する壁を有し、該壁と鉛直線とのなす角度が1.
3゜以上3.9゜以内であれば問題ないが、モノシラン
の変換率をより高率とするためにはこの角度は3.0゜
以上3.9゜以内がより望ましい。In the reactor of the present invention, even if the bubbles of the cracking gas (silane and hydrogen) formed in the fluidized bed are larger than the diameter of the reaction vessel, the reactor diameter increases as the bubbles rise. Above a certain height, the bubbles are below the reactor diameter, slug flow is eliminated and a high conversion of silane is obtained. Moreover, the gas linear velocity in the upper part of the fluidized bed is 2 ×
Since Umf ≦ U, the silicon particles are not condensed due to the decrease in the gas linear velocity. The shape of the reactor has a wall that forms a cone that opens upward, and the angle between the wall and the vertical line is 1.
There is no problem if it is 3 ° or more and 3.9 ° or less, but it is more preferable that this angle is 3.0 ° or more and 3.9 ° or less in order to make the conversion rate of monosilane higher.
【0013】[0013]
【発明の効果】以上の説明により理解されるように、本
発明によれば、相当広い粒子径の範囲であっても、また
反応器直径が相当に小さいものであってもシリコン粒子
の凝結がおこらず、シランのシリコンへの変換率も高率
が得られると言う効果を発揮することができる。As can be understood from the above description, according to the present invention, even if the particle diameter is in a considerably wide range, or even if the reactor diameter is considerably small, the silicon particles are not condensed. It is possible to exert the effect that a high conversion rate of silane to silicon can be obtained without any occurrence.
【0014】[0014]
実施例1 図2に示す態様により下記条件で多結晶シリコンを製造
した。 反応器の形状:上開きの錐体を形成する壁を有し、該壁
と鉛直線とのなす角度が 3.0゜ 粒子平均径:1000μm 反応温度:650℃ 原料ガスのモノシラン濃度:10mol% 原料ガス(モノシランと水素)線速:2m/sec シリコン製造において、シリコン粒子が凝結し、反応器
が閉塞することもなく、さらに、モノシランのシリコン
への変換率は定常的に99mol%以上で3カ月連続稼
働した。Example 1 Polycrystalline silicon was manufactured under the following conditions according to the embodiment shown in FIG. Shape of reactor: It has a wall that forms an upward-opening cone, and the angle between the wall and the vertical line is 3.0 ° Particle average diameter: 1000 μm Reaction temperature: 650 ° C. Concentration of monosilane in the source gas: 10 mol% Raw material gas (monosilane and hydrogen) Linear velocity: 2 m / sec In silicon production, silicon particles do not coagulate and the reactor is not clogged, and the conversion rate of monosilane to silicon is steadily 99 mol% or more. It has been operating continuously for a month.
【0015】比較例1 反応管の形状が上開きの錐体を形成する壁を有し、しか
しながら該壁と鉛直線とのなす角度は4.0゜であっ
た。そのこと以外は実施例1と同様に反応を行ったとこ
ろ、モノシランを反応器に導入すると同時に流動床上部
でシリコン粒子の凝結が起こり反応器が閉塞した。Comparative Example 1 The shape of the reaction tube had a wall forming an upwardly-opened cone, but the angle formed by the wall and the vertical line was 4.0 °. Other than that, when the reaction was carried out in the same manner as in Example 1, the silicon silane was condensed in the upper part of the fluidized bed at the same time when monosilane was introduced into the reactor, and the reactor was blocked.
【0016】実施例2 反応管の形状が上開きの錐体を形成する壁を有し、該壁
と鉛直線とのなす角度が1.6゜以外は実施例1と同様
に反応を行ったところ、モノシランのシリコンへの変換
率は70mol%だった。Example 2 The reaction was carried out in the same manner as in Example 1 except that the shape of the reaction tube had a wall forming an upward-opening cone and the angle between the wall and the vertical line was 1.6 °. However, the conversion rate of monosilane to silicon was 70 mol%.
【図1】分解用ガス中のシラン濃度と分解ガス線速との
相関において、シリコン粒子の凝結が起る場合と起らな
い場合を示す図である。FIG. 1 is a diagram showing a correlation between a silane concentration in a decomposition gas and a decomposition gas linear velocity when condensation of silicon particles occurs and when condensation does not occur.
【図2】本発明の流動床反応器の一実施態様の概略断面
図である。FIG. 2 is a schematic cross-sectional view of one embodiment of the fluidized bed reactor of the present invention.
○印:シリコン粒子の凝結なし ★印:シリコン粒子の凝結あり 1:反応容器 2:ヒータ 3:シリコン粒子供給管 4:モノシランガス導入口 5:水素ガス導入管 6:粒状シリコン抜出管 7:ガス抜き管 8:ガス分散板 9:ガスサンプリング口 10:ガスクロマトグラフ ○: No condensation of silicon particles ★: Condensation of silicon particles 1: Reaction vessel 2: Heater 3: Silicon particle supply pipe 4: Monosilane gas inlet port 5: Hydrogen gas inlet pipe 6: Granular silicon extraction pipe 7: Gas Vent pipe 8: Gas dispersion plate 9: Gas sampling port 10: Gas chromatograph
Claims (1)
てこの壁が鉛直線となす角度が1.3〜3.9゜の範囲に
あることを特徴とするモノシラン分解用流動床反応器。1. A fluidized bed for decomposing monosilane, characterized in that it has a wall forming an upward-opening cone, and the angle between this wall and a vertical line is in the range of 1.3 to 3.9 °. Reactor.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17648094A JPH0840717A (en) | 1994-07-28 | 1994-07-28 | Fluidized bed reactor for monosilane decomposition |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17648094A JPH0840717A (en) | 1994-07-28 | 1994-07-28 | Fluidized bed reactor for monosilane decomposition |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0840717A true JPH0840717A (en) | 1996-02-13 |
Family
ID=16014411
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP17648094A Withdrawn JPH0840717A (en) | 1994-07-28 | 1994-07-28 | Fluidized bed reactor for monosilane decomposition |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0840717A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2010227805A (en) * | 2009-03-26 | 2010-10-14 | Panasonic Electric Works Co Ltd | Continuous processing equipment |
| KR20150048772A (en) * | 2012-08-29 | 2015-05-07 | 헴로크세미컨덕터코포레이션 | Tapered fluidized bed reactor and process for its use |
-
1994
- 1994-07-28 JP JP17648094A patent/JPH0840717A/en not_active Withdrawn
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2010227805A (en) * | 2009-03-26 | 2010-10-14 | Panasonic Electric Works Co Ltd | Continuous processing equipment |
| KR20150048772A (en) * | 2012-08-29 | 2015-05-07 | 헴로크세미컨덕터코포레이션 | Tapered fluidized bed reactor and process for its use |
| JP2015529185A (en) * | 2012-08-29 | 2015-10-05 | ヘムロック・セミコンダクター・コーポレーション | Tapered fluidized bed reactor and process for its use |
| US10105669B2 (en) | 2012-08-29 | 2018-10-23 | Hemlock Semiconductor Operations Llc | Tapered fluidized bed reactor and process for its use |
| US10265671B2 (en) | 2012-08-29 | 2019-04-23 | Hemlock Semiconductor Operations Llc | Tapered fluidized bed reactor and process for its use |
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