JPH03183683A - Electric furnace - Google Patents

Electric furnace

Info

Publication number
JPH03183683A
JPH03183683A JP31879589A JP31879589A JPH03183683A JP H03183683 A JPH03183683 A JP H03183683A JP 31879589 A JP31879589 A JP 31879589A JP 31879589 A JP31879589 A JP 31879589A JP H03183683 A JPH03183683 A JP H03183683A
Authority
JP
Japan
Prior art keywords
heater
single crystal
electric furnace
temp
melt zone
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.)
Granted
Application number
JP31879589A
Other languages
Japanese (ja)
Other versions
JPH0579637B2 (en
Inventor
Yoshio Fujino
芳男 藤野
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.)
NEC Corp
Original Assignee
NEC Corp
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 NEC Corp filed Critical NEC Corp
Priority to JP31879589A priority Critical patent/JPH03183683A/en
Publication of JPH03183683A publication Critical patent/JPH03183683A/en
Publication of JPH0579637B2 publication Critical patent/JPH0579637B2/ja
Granted legal-status Critical Current

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

Abstract

PURPOSE:To allow stable temp. control and to prevent the fluctuation in compsn. of a single crystal by connecting two pieces of specific heaters in series so as to avoid the thermal interference thereof with each other and disposing these heaters in an electric furnace for growing the single crystal by a floating zone method. CONSTITUTION:The 1st heater 14a for forming the melt zone having a heating temp. range of a narrow peak characteristic is provided in the electric furnace for growing the single crystal by the floating zone method. Further, the 2nd heater 14b for temp. control having a broad and flat heating temp. range is provided. The 1st heater 14a and the 2nd heater 14b are so disposed that the heaters are not thermally interfered with each other and are connected electrically in series. The raw materials 1 in a quartz ampoule 7 are heated and melted by the heater 14a to form the melt zone 3 and while the temp. is controlled by the heater 14b, the single crystal 2 is grown by the floating zone method.

Description

【発明の詳細な説明】 [産業上の利用分野1 本発明は電気炉に関し、さらに詳しくはフローティング
ゾーン法で単結晶を育成する際に用いる電気炉に関する
DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field 1] The present invention relates to an electric furnace, and more particularly to an electric furnace used for growing single crystals by the floating zone method.

[従来の技術] フローティングゾーン法で単結晶を育成するのに用いる
電気炉はbO熱の方法によって高周波炉と抵抗炉とに分
けられる。高周波炉は電源に費用がかかり、場所もやや
広いところを要求される。抵抗炉は実験者が自分の計画
どおり手作りできる良さかあり、電源も安価で場所もそ
れ程広くなくてすむ等の長所がある。
[Prior Art] Electric furnaces used to grow single crystals by the floating zone method are classified into high frequency furnaces and resistance furnaces depending on the bO heating method. High frequency furnaces require an expensive power source and a rather large space. Resistance furnaces have the advantage that experimenters can make them by hand according to their own plans, the power supply is cheap, and they do not require a large space.

フローティングゾーン法による電気炉の概略は第3図に
示すとありで、第3図(a)のように原料1と単結晶2
の間にメルトゾーン3を形成するためにヒータ4を設け
るが、このヒータによって形成される温度分布は第3図
(b)のようにピーク性の狭い加熱範囲Aのものとなる
The outline of the electric furnace using the floating zone method is shown in Figure 3.As shown in Figure 3(a), raw material 1 and single crystal 2 are
A heater 4 is provided to form a melt zone 3 between the two, but the temperature distribution formed by this heater is in a heating range A with a narrow peak as shown in FIG. 3(b).

[発明が解決しようとする課題] 育成される結晶の組成を均一にするには、ヒタの加熱で
作られるメルトゾーンの温度が所定の値に長時間保持さ
れなければならない。また、温度分布もピーク性の幅狭
いものでなければならない。抵抗炉の場合はこの温度制
御のために熱電対5が設置される。
[Problems to be Solved by the Invention] In order to make the composition of the grown crystals uniform, the temperature of the melt zone created by heating the heater must be maintained at a predetermined value for a long time. Furthermore, the temperature distribution must also have a narrow peak. In the case of a resistance furnace, a thermocouple 5 is installed for this temperature control.

しかしながら、温度分布がピーク性で平坦な部分がない
ため、温度制御器の時定数の許容範囲が狭くなり正確な
時定数か得にくいため、出力がいわゆるハンチングを起
こし不安定となる。そして結果として、メルトゾーンの
温度が所定の値に安定しなくなるという欠点があった。
However, since the temperature distribution has peaks and no flat parts, the allowable range of the time constant of the temperature controller becomes narrow and it is difficult to obtain an accurate time constant, resulting in so-called hunting in the output and making it unstable. As a result, there was a drawback that the temperature of the melt zone was not stabilized at a predetermined value.

これを安定させるために、温度分布に平坦性を持たせる
方法かあるが、それはメルトゾーン3の幅(第3図では
縦方向の長ざ)を大きくしなければならず、このことは
結晶組成のずれを招くことになる。ちなみにメルトゾー
ンの幅は、一般にゾーンの直径とほぼ同じか、それ以下
としている。
In order to stabilize this, there is a method to make the temperature distribution flat, but this requires increasing the width of melt zone 3 (the length in the vertical direction in Figure 3), which means that the crystal composition This will lead to misalignment. Incidentally, the width of the melt zone is generally set to be approximately the same as or less than the diameter of the zone.

本発明は以上述べたような従来の課題を解決するために
なされたもので、メルトゾーンの温度が安定して組成変
動の極めて少ない単結晶を得ることのできる単結晶育成
用の電気炉を提供することを目的とする。
The present invention has been made in order to solve the conventional problems as described above, and provides an electric furnace for growing single crystals in which the temperature of the melt zone is stable and a single crystal with extremely little compositional fluctuation can be obtained. The purpose is to

[課題を解決するための手段] 本発明は、70−ティングゾーン法による単結晶育成に
用いられる電気炉において、幅狭いピーク性の加熱温度
範囲を有するメルトゾーン形成相の第1のヒータと、幅
広い平坦な加熱温度範囲を有する温度制御用の第2のヒ
ータとを備え、該第1のヒータと第2のヒータは熱的に
干渉せず、かつ電気的に直列に接続するように配置した
ことを特徴とする電気炉である。
[Means for Solving the Problems] The present invention provides an electric furnace used for single crystal growth by the 70-ting zone method, which includes: a first heater for a melt zone forming phase having a narrow peak heating temperature range; and a second heater for temperature control having a wide flat heating temperature range, and the first heater and the second heater are arranged so as not to interfere thermally and to be electrically connected in series. This electric furnace is characterized by:

[作用] 第1図は本発明の電気炉について、実施例を兼ねてその
構成を示したものである。同図に示すように、本発明の
電気炉においては、ヒータ構成は二つのヒータ14aお
よび14bからなっており、そのうち第1のヒータ14
aはゾーンメルト用で従来どおり単結晶2と原料1の間
にメルトゾーン3を形成するための幅狭いピーク性の加
熱範囲Aを持ち、もう一つの第2のヒータ14bは温度
制御用で幅広い平坦な加熱範囲Bを持ち、ヒータ14a
とは熱的に干渉しないよう充分な距離をもって直列に配
置されている。温度制御用の熱電対15bはヒタ14b
の傍に配置され、またヒータ14aの傍にはモニタ用の
熱電対15aか設置されている。
[Function] FIG. 1 shows the structure of the electric furnace of the present invention, which also serves as an embodiment. As shown in the figure, in the electric furnace of the present invention, the heater configuration consists of two heaters 14a and 14b, of which the first heater 14
The heater 14a is for zone melting and has a narrow peak heating range A for forming the melt zone 3 between the single crystal 2 and the raw material 1 as before, and the other second heater 14b is for temperature control and has a wide heating range A. The heater 14a has a flat heating range B.
and are placed in series with a sufficient distance to avoid thermal interference. The thermocouple 15b for temperature control is the heater 14b.
A monitoring thermocouple 15a is also installed near the heater 14a.

以上のように構成された電気炉を用いた結晶育成は次の
ように行う。メルトゾーン3が所定の温度になるように
モニタ熱電対15aを児ながら温度制御用ヒータ14b
に電力を供給し、メルトゾーン3が所定の温度になった
ならば通常のごとくフローティングゾーン法で単結晶育
成の手順を行えばよい。
Crystal growth using the electric furnace configured as described above is performed as follows. The temperature control heater 14b is connected to the monitor thermocouple 15a so that the melt zone 3 reaches a predetermined temperature.
When the temperature of the melt zone 3 reaches a predetermined temperature, single crystal growth can be carried out using the floating zone method as usual.

ヒータ14bは幅広い平坦な加熱範囲Bを持っているの
で温度制御器の時定数の許容範囲が広く、極めて安定な
温度制御が行われる。そのためヒータ14bを流れる電
流は安定しており、したがってメルトゾーン形成相のヒ
ータ14aに流れる電流も安定なため、メルトゾーン3
の温度も極めて安定な温度が確保できる。
Since the heater 14b has a wide and flat heating range B, the allowable range of the time constant of the temperature controller is wide, and extremely stable temperature control is performed. Therefore, the current flowing through the heater 14b is stable, and therefore the current flowing through the heater 14a during the melt zone formation phase is also stable.
An extremely stable temperature can also be ensured.

[実施例] 次に本発明の実施例について詳細に説明する。[Example] Next, embodiments of the present invention will be described in detail.

単結晶育成の対象としたのはn−Vl族化合物半導体の
テルル化水銀カドミウム(口go8Cd□、2Te)で
ある。原料としてテルル化水銀(目qTe)とテルル化
カドミウム(CdTe)をモル比で4=1となるように
混合・融解して多結晶化したものを用いた。メルトゾー
ン用の材料はテルルを過剰にしたテルル化水銀カドミウ
ムであって、融解温度が500’Cとなるように組成を
調整した。また、種子結晶としてはテルル化カドミウム
(CdTe)の(111)面が水平面となるように調整
されたものを用いた。これら三つを第2図に示すように
、内径10 mm、長さ150 mmの石英アンプル7
に種子結晶6、メルトゾーン材料13、原料1の順に重
ねて真空封入した。
The target for single crystal growth was mercury cadmium telluride (g08Cd□, 2Te), which is an n-Vl group compound semiconductor. As a raw material, mercury telluride (Te) and cadmium telluride (CdTe) were mixed and melted in a molar ratio of 4=1 to form polycrystals. The material for the melt zone was mercury cadmium telluride with an excess of tellurium, and the composition was adjusted to have a melting temperature of 500'C. Further, as a seed crystal, a crystal of cadmium telluride (CdTe) adjusted so that the (111) plane was a horizontal plane was used. As shown in Figure 2, these three are placed in a quartz ampoule 7 with an inner diameter of 10 mm and a length of 150 mm.
Seed crystal 6, melt zone material 13, and raw material 1 were layered in this order and vacuum sealed.

このように準備したアンプルを第1図(a)のように二
つのヒータ14aおよび14bからなる抵抗式の電気炉
内に吊し、モニタ熱電対15aが500℃を示すように
制御用ヒータ14bを制御した。この時、制御用熱電対
15bは515°Cを示し、温度の安定度は±0.1°
Cて極めて安定していた。モニタ熱電対15aは±0.
4°Cのゆらぎがあったか、従来法の1710以下の安
定度であった。このゆらぎはヒータ付近の空気の対流に
よるものであると考えられる。
The ampoule prepared in this manner is suspended in a resistance type electric furnace consisting of two heaters 14a and 14b as shown in FIG. controlled. At this time, the control thermocouple 15b indicates 515°C, and the temperature stability is ±0.1°.
C was extremely stable. The monitor thermocouple 15a is ±0.
There was a fluctuation of 4°C, or the stability was lower than 1710 of the conventional method. This fluctuation is thought to be due to air convection near the heater.

単結晶の育成はメルトゾーンの移動か1時間当たり0.
3mmと唸るような早さでアンプル7をゆつくり吊り下
げていった。原料の長さ60 nonをメルトゾーン3
が完全に通過するまで、即ちメルトゾーン3が原料の上
端に達するまで行った。
Single crystal growth is achieved through the movement of the melt zone or at 0.00% per hour.
Ampoule 7 was slowly suspended at an astounding speed of 3mm. Raw material length 60 non melt zone 3
The process was continued until the melt had completely passed through, that is, until the melt zone 3 reached the upper end of the raw material.

終了後、育li、された単結晶をアンプルから取り出し
、スライスして長さ方向について組成の変動(水銀とカ
ドミウムのモル比の変化の様子)を調べたところ、従来
法の1/10程度に小さくなっていることか判明した。
After the cultivation, the grown single crystal was removed from the ampoule, sliced, and examined for changes in composition (changes in the molar ratio of mercury and cadmium) in the length direction. It turned out that it was getting smaller.

このことから加熱用のヒータの他に温度制御用のヒータ
を設けたことによる効果か明らかになった。
From this, it became clear that the effect was due to the provision of a heater for temperature control in addition to the heater for heating.

[発明の効果1 以上詳述したように、本発明の電気炉を用いて抵抗式の
フローティングゾーン式単結晶育成法により単結晶を育
成すると、安定な温度制御が可能となり、その結果、メ
ルトゾーンの温度が安定となって組成変動の極めて少な
い単結晶を得ることができる。
[Advantageous Effects of the Invention 1] As detailed above, when a single crystal is grown by the resistance floating zone single crystal growth method using the electric furnace of the present invention, stable temperature control becomes possible, and as a result, the melt zone The temperature becomes stable and a single crystal with very little compositional fluctuation can be obtained.

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

第1図は本発明の電気炉の一実施例の概略構成図と炉内
の温度分布図、第2図は石英アンプル内の原料の構成図
、第3図は従来技術による電気炉の一例の概略構成図と
炉内の温度分布図である。 1・・・原料       2・・・単結晶3・・・メ
ルトゾーン 4、14a 、 14b ・L−タ 5、15a 、 15b −・・熱電対6・・・種子結
晶     7・・・石英アンプル13・・・メルトゾ
ーン材料
Fig. 1 is a schematic diagram of an embodiment of the electric furnace of the present invention and a temperature distribution diagram in the furnace, Fig. 2 is a diagram of the composition of raw materials in a quartz ampoule, and Fig. 3 is an example of an electric furnace according to the prior art. They are a schematic configuration diagram and a temperature distribution diagram inside the furnace. 1... Raw material 2... Single crystal 3... Melt zone 4, 14a, 14b - L-ta 5, 15a, 15b -... Thermocouple 6... Seed crystal 7... Quartz ampoule 13.・・Melt zone material

Claims (1)

【特許請求の範囲】[Claims] (1)フローティングゾーン法による単結晶育成に用い
られる電気炉において、幅狭いピーク性の加熱温度範囲
を有するメルトゾーン形成用の第1のヒータと、幅広い
平坦な加熱温度範囲を有する温度制御用の第2のヒータ
とを備え、該第1のヒータと第2のヒータは熱的に干渉
せず、かつ電気的に直列に接続するように配置したこと
を特徴とする電気炉。
(1) In an electric furnace used for single crystal growth using the floating zone method, a first heater for forming a melt zone has a narrow peak heating temperature range, and a first heater for temperature control has a wide flat heating temperature range. An electric furnace comprising: a second heater; the first heater and the second heater are arranged so as not to thermally interfere with each other and to be electrically connected in series.
JP31879589A 1989-12-11 1989-12-11 Electric furnace Granted JPH03183683A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP31879589A JPH03183683A (en) 1989-12-11 1989-12-11 Electric furnace

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP31879589A JPH03183683A (en) 1989-12-11 1989-12-11 Electric furnace

Publications (2)

Publication Number Publication Date
JPH03183683A true JPH03183683A (en) 1991-08-09
JPH0579637B2 JPH0579637B2 (en) 1993-11-04

Family

ID=18103030

Family Applications (1)

Application Number Title Priority Date Filing Date
JP31879589A Granted JPH03183683A (en) 1989-12-11 1989-12-11 Electric furnace

Country Status (1)

Country Link
JP (1) JPH03183683A (en)

Also Published As

Publication number Publication date
JPH0579637B2 (en) 1993-11-04

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