JPH034516A - Molecular beam source - Google Patents
Molecular beam sourceInfo
- Publication number
- JPH034516A JPH034516A JP13998289A JP13998289A JPH034516A JP H034516 A JPH034516 A JP H034516A JP 13998289 A JP13998289 A JP 13998289A JP 13998289 A JP13998289 A JP 13998289A JP H034516 A JPH034516 A JP H034516A
- Authority
- JP
- Japan
- Prior art keywords
- molecular beam
- shutter
- beam source
- crucible
- open end
- 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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- Physical Deposition Of Substances That Are Components Of Semiconductor Devices (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
〔発明の目的〕
(産業上の利用分野)
本発明は超格子等の半導体多層薄膜構造の結晶を成長す
る分子線エピタキシャル装置の分子線源に関する。DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial Application Field) The present invention relates to a molecular beam source for a molecular beam epitaxial apparatus for growing crystals of a semiconductor multilayer thin film structure such as a superlattice.
(従来の技術)
分子線二ピタキシャル成長法C以下MBE法と略記する
)は、真空容器内で分子g源から射出した分子線を半導
体基板に照射して半導体結晶膜を成長する技術である6
MBE法で成長した多層薄膜構造の結晶(−層あたりの
膜厚は数人から数百人)を用いることにより優れた特性
の半導体素子を製作することができる。(Prior art) Molecular beam bipitaxial growth method C (hereinafter abbreviated as MBE method) is a technology in which a semiconductor substrate is irradiated with a molecular beam emitted from a molecular g source in a vacuum chamber to grow a semiconductor crystal film6. Semiconductor elements with excellent characteristics can be manufactured by using crystals with a multilayer thin film structure grown by the MBE method (thickness per layer ranges from several layers to several hundred layers).
このような半導体結晶を製作するためには、結晶の成長
速度及び膜厚を所望の値に精密に制御する必要がある。In order to manufacture such a semiconductor crystal, it is necessary to precisely control the crystal growth rate and film thickness to desired values.
従来の分子線源を配置した分子線エピタキシャル成長装
置(以下HBE装置と略記する)の−例を第3図に示し
た断面図によって説明する真空容器101内に゛は、−
例としてGaおよびAsの分子線源102a、 102
bが設置され、前記分子線源肋、肋に対向する位置には
、半導体基板の例えばGaAs基板103を保持した半
導体基板ホルダ104が設けられている。An example of a molecular beam epitaxial growth apparatus (hereinafter abbreviated as HBE apparatus) equipped with a conventional molecular beam source is explained with reference to the cross-sectional view shown in FIG.
For example, Ga and As molecular beam sources 102a, 102
b is installed, and a semiconductor substrate holder 104 holding a semiconductor substrate, for example, a GaAs substrate 103, is provided at a position facing the molecular beam source rib and the rib.
前記分子線源■ハ、胆並は、分子線材料のGa105a
、 As 105bを入れた各るつぼl06a、 10
6bと、前記分子線材料を加熱するための各ヒータ 1
07a。The molecular beam source (c) is the molecular beam material Ga105a.
, each crucible containing As 105b l06a, 10
6b, and each heater 1 for heating the molecular beam material.
07a.
107bと、熱効率を向上させるための例えば阿0の熱
反射板108a、 108bと、温度制御のための熱電
対109a、 109bと、分子線を遮断するための板
状のシャッタ110a、 110bおよびこれらのシャ
ッタを回転させるシャッタ回転軸111aおよび111
bで構成されている。前記シャッタ板110a、 11
0bは、前記各るつぼ106a、 106bの分子線射
出口(開口部) 116a。107b, heat reflecting plates 108a and 108b, for example, A0, for improving thermal efficiency, thermocouples 109a and 109b for temperature control, plate-shaped shutters 110a and 110b for blocking molecular beams, and these. Shutter rotation shafts 111a and 111 that rotate the shutter
It is composed of b. The shutter plates 110a, 11
0b is a molecular beam injection port (opening) 116a of each crucible 106a, 106b.
116bにこれらの分子線射出口(開口面)と平行に配
置されている。116b is arranged parallel to these molecular beam exit ports (aperture planes).
上記のMBE装置での成長速度及び膜厚の制御は次の手
順で行なわれる。まず、この成長に先立ち試験的な結晶
成長を行なう。結晶成長後結晶を装置から取り出し、結
晶をへき関し、その断面にステンエッチングを施し成長
層境界線を見易くした後、走査型電子顕微鏡(SEM)
を用いて膜厚を測定し、その膜厚と成長時間から成長速
度を平均的に算出、決定する。その成長速度を基に、こ
れから成長を行おうとする結晶の膜厚に対応する成長時
間を計算し、シャツタ板の開閉により所望の膜厚の結晶
を成長する。The growth rate and film thickness are controlled by the following procedure in the above MBE apparatus. First, prior to this growth, experimental crystal growth is performed. After crystal growth, the crystal was removed from the apparatus, separated, and its cross section was etched to make it easier to see the growth layer boundaries, and then subjected to scanning electron microscopy (SEM).
The film thickness is measured using a method, and the growth rate is averaged and determined from the film thickness and growth time. Based on the growth rate, a growth time corresponding to the thickness of the crystal to be grown is calculated, and the crystal of the desired thickness is grown by opening and closing the shirt shirt plate.
上記のようなシャツタ板を有する分子線源においてシャ
ツタ板を開いた直後からの分子線強度の時間変化の一例
を第4図に示す。分子線強度が一定値となるまでに約3
分を要している。この原因は、前記シャツタ板を閉じて
いる状態ではシャツタ板からの熱輻射の反射により、分
子線材料表面の温度が上昇するために、シャッタ開放直
後の分子線強度が増加し、その後るつぼ内が熱平衡に達
するまでにある時間を有することによる。FIG. 4 shows an example of the temporal change in the molecular beam intensity immediately after opening the shutter plate in a molecular beam source having the shutter plate as described above. It takes about 30 minutes for the molecular beam intensity to reach a constant value.
It takes minutes. The reason for this is that when the shutter plate is closed, the temperature of the surface of the molecular beam material increases due to the reflection of thermal radiation from the shutter plate, so the molecular beam intensity increases immediately after the shutter is opened, and then the inside of the crucible increases. By having a certain amount of time to reach thermal equilibrium.
従って叙上の成長方法で説明したように、平均的な成長
速度を基に膜厚を制御する場合は、設定した膜厚と実際
に成長した膜厚との間に誤差が生ずる。特に超格子薄膜
等微細な構造を有する結晶を成長する場合は精密な膜厚
制御を行うのが困難となる。Therefore, as explained in the above growth method, when controlling the film thickness based on the average growth rate, an error occurs between the set film thickness and the actually grown film thickness. In particular, when growing crystals with fine structures such as superlattice thin films, it is difficult to precisely control the film thickness.
(発明が解決しようとする課題)
以上述べたようにシャツタ板をるつぼの分子線射出口(
開口面)と平行に配置したMBE装置では、前記シャツ
タ板開放直後に分子線強度が変動するため、膜厚の精密
な制御を行うのが困難である。(Problems to be Solved by the Invention) As mentioned above, the shatter plate is connected to the molecular beam injection port of the crucible (
In an MBE device arranged parallel to the opening plane), the molecular beam intensity fluctuates immediately after the shutter plate is opened, making it difficult to precisely control the film thickness.
本発明は上記の欠点を除去すべくなされたもので、微細
な構造を持つ結晶の成長を制御性良く行ない得るシャッ
タ構造を有する分子線源を提供することを目的とする。The present invention has been made to eliminate the above-mentioned drawbacks, and an object of the present invention is to provide a molecular beam source having a shutter structure that allows growth of crystals having a fine structure with good controllability.
(課題を解決するための手段)
本発明にかかる分子線源は、真空容器内に分子線源のる
つぼから射出した分子線をシャッタ機構により断続させ
て半導体基板に照射しこの半導体基板の半導体結晶膜を
成長させる分子線エピタキシャル成長装置の分子線源に
おいて、シャッタが屈曲された管型で、その一方の開端
の中心軸を除く部位を回転軸とする回転によりこの開端
が前記るつぼの分子線射出口に対向することを特徴とす
る。(Means for Solving the Problems) The molecular beam source according to the present invention is capable of intermittent molecular beams ejected from a crucible of the molecular beam source into a vacuum container using a shutter mechanism to irradiate a semiconductor substrate with semiconductor crystals of the semiconductor substrate. In a molecular beam source of a molecular beam epitaxial growth apparatus for growing a film, the shutter is in the shape of a bent tube, and one open end of the shutter rotates around a rotation axis other than the center axis, so that this open end becomes the molecular beam exit of the crucible. It is characterized by facing.
(作 用)
本発明は分子線源において、分子線源のるつぼから半導
体基板に至る分子線を断続させるシャッタを屈曲された
管型に形成し、シャッタによる閉止時に、るつぼの分子
線射出口(開口面)に一方の開端を対向させ、他方の開
端ば半導体基板と異なる方向に指向させてこの半導体基
板に分子線が入射しないように構成した。かかる構成に
より、シャッタによる熱輻射で分子線材料表面の温度上
昇を低減させることができる。これにより、従来問題で
あったシャッタ開放直後の分子線強度の変動を抑えるこ
とができる。(Function) The present invention provides a molecular beam source in which a shutter for cutting off the molecular beam from the crucible of the molecular beam source to the semiconductor substrate is formed into a bent tube shape, and when the shutter is closed, the molecular beam exit port ( One open end was made to face the open end (opening surface), and the other open end was oriented in a direction different from that of the semiconductor substrate, so that the molecular beam would not be incident on the semiconductor substrate. With this configuration, it is possible to reduce the temperature rise on the surface of the molecular beam material due to thermal radiation caused by the shutter. This makes it possible to suppress fluctuations in the molecular beam intensity immediately after the shutter is opened, which has been a problem in the past.
(実施例)
以下、本発明の一実施例につき図面を参照(2゜で説明
する。なお、説明において、従来と変わらない部分につ
いては図面に従来と同じ符号を付けて示し、説明を省略
する。(Embodiment) Hereinafter, an embodiment of the present invention will be explained with reference to the drawings (described in 2 degrees. In the explanation, parts that are the same as the conventional ones will be indicated with the same reference numerals as in the conventional drawings, and the explanation will be omitted. .
第1図に本発明にかかる分子線源を備える分子線エピタ
キシャル成長装置によりGaAsをエピタキシャル成長
する場合の該装置の要部を断面図で示す。FIG. 1 shows a cross-sectional view of the main parts of a molecular beam epitaxial growth apparatus equipped with a molecular beam source according to the present invention when epitaxially growing GaAs.
第1図に示すように、分子線源10a、 10bの改良
された点は、分子線材料のGa 105aを入れたるっ
ぽ1060と、As 105bを入れたるつぼ106b
の各分子線射出口(開口面) 1i6a、 116bの
直前にシャツタ+1.a、 llbがシャッタ回転軸1
2a、 12bに取付されて配置されている。これらの
シャッタIla、 Ilbはいずれも一例として材質は
Moで、その形状は屈曲された管型になり、その一方の
開端21a、 21bの中心軸Xa、 Xbを除く部位
にシャッタ回転軸12a、 12bが取付され、回転軸
の回転によって一方の開端21a。As shown in FIG. 1, the improvements to the molecular beam sources 10a and 10b include a luppo 1060 containing the molecular beam material Ga 105a and a crucible 106b containing As 105b.
Immediately before each molecular beam exit port (opening surface) 1i6a, 116b, there is a shutter +1. a, llb is shutter rotation axis 1
2a and 12b. These shutters Ila and Ilb are all made of Mo, for example, and have a bent tube shape, and have shutter rotation axes 12a and 12b at the opening ends 21a and 21b, except for the central axes Xa and Xb. is attached, and one open end 21a is opened by rotation of the rotating shaft.
21bがるつぼ106a、 106bの各分子線射出口
(開口面)に対向し、他方の開端31a、 31bはシ
ャッタ内−を通る分子線が基板へ入射しない方向へ指向
され机
次に上述の分子線の機能について説明する。21b faces each molecular beam exit port (opening surface) of the crucibles 106a and 106b, and the other open ends 31a and 31b are oriented in a direction in which the molecular beam passing through the shutter does not enter the substrate, so that the molecular beam described above is Explain the functions of.
シャッタfla、 11.bが閉じた状態では、分子線
材料105a、 105bからの蒸発分子はるつぼ10
6a、 106bの分子線射出口(開口部) 116a
、 1]、6bを経てシャッタlla、 llbの開端
2La、 21bより内部に入り、シャッタ内を通過し
て真空容器内に射出される。このときシャッタIla、
Ilbは屈曲されているため、GaAs基板103に
は到達しない、更にシャッタ1】a。Shutter fla, 11. When b is closed, the evaporated molecules from the molecular beam materials 105a and 105b are transferred to the crucible 10.
Molecular beam injection port (opening) 116a of 6a, 106b
, 1], 6b, enters the interior through the open ends 2La, 21b of the shutters lla, llb, passes through the shutters, and is injected into the vacuum container. At this time, the shutter Ila,
Since Ilb is bent, it does not reach the GaAs substrate 103, and the shutter 1]a.
1 ]、bが管型であるためシャッタからの熱輻射によ
る分子線材料表面の温度上昇は抑えられている。1] and b are tubular, so the temperature rise on the surface of the molecular beam material due to thermal radiation from the shutter is suppressed.
したがってシャッタlla、 Ilbを開放した場合、
るっぽ106a、 106b内の蒸気圧は閉じた状態の
時に比へてほとんど変化しないので、第2図に示すよう
に、開放直後の分子線強度の変動が大幅に減少される。Therefore, when shutters lla and Ilb are opened,
Since the vapor pressure inside the Ruppo 106a, 106b hardly changes compared to when the Ruppo 106a and 106b are in the closed state, fluctuations in the molecular beam intensity immediately after opening are greatly reduced, as shown in FIG.
なお、管型のシャッタ形状は、上述の実施例第1図に示
したものに限定されるものではなく、方の開口部がるつ
ぼの分子線射出口に、他の一方の開口部は分子線が基板
へ到達しないような方向へ向けられておれば、他の形状
であっても構わないことは上述の説明から明らかであろ
う。Note that the shape of the tube-shaped shutter is not limited to that shown in FIG. It will be clear from the above description that other shapes are possible as long as they are oriented in a direction that prevents them from reaching the substrate.
また、本実施例ではGaAsの場合について述べたが、
AQGaAs等の他の結晶成長についても適用できる。In addition, although the case of GaAs was described in this example,
It can also be applied to other crystal growths such as AQGaAs.
以上述べたように本発明によれば、シャッタ開放直後の
分子線強度の変動を抑えることができ、微細な構造をを
持つ半導体結晶の膜厚を精密に制御できる分子線源を提
供できる。As described above, according to the present invention, it is possible to provide a molecular beam source that can suppress fluctuations in molecular beam intensity immediately after the shutter is opened and can precisely control the film thickness of a semiconductor crystal having a fine structure.
第1図は本発明の一実施例を説明するためのMBE装置
の要部の断面図、第2図は第1図に示される実施例にお
いて測定されたシャッタ開放直後の分子線強度の時間変
化の一例を示す線図、第3図は従来のMBE装置の要部
の断面図、第4図は第3図に示される例において測定さ
れたシャッタ開放直後の分子線強度の時間変化の一例を
示す線図である。
10a、 10b・・・分子線源 11a、 I]、
b・・・シャッタ21a、 21b・・・シャッタの一
方のG[、Xa、 Xb・・・シャンター 方の開端の
中心軸+06a、 106b−るつぼFIG. 1 is a cross-sectional view of the main parts of an MBE apparatus for explaining an embodiment of the present invention, and FIG. 2 is a temporal change in molecular beam intensity immediately after the shutter is opened, measured in the embodiment shown in FIG. 1. A line diagram showing an example, FIG. 3 is a cross-sectional view of the main part of a conventional MBE apparatus, and FIG. 4 shows an example of the temporal change in molecular beam intensity immediately after the shutter is opened in the example shown in FIG. FIG. 10a, 10b... molecular beam source 11a, I],
b...Shutters 21a, 21b...One of the shutters G[, Xa, Xb...Central axis of the open end of the shunter +06a, 106b-crucible
Claims (1)
シャッタ機構により断続させて半導体基板に照射しこの
半導体基板に半導体結晶膜を成長させる分子線エピタキ
シャル成長装置の分子線源において、シャッタが屈曲さ
れた管型で、その一方の開端の中心軸を除く部位を回転
軸とする回転によりこの開端が前記るつぼの分子線射出
口に対向することを特徴とする分子線源。In a molecular beam source of a molecular beam epitaxial growth system in which a semiconductor substrate is irradiated with a molecular beam emitted from a crucible of a molecular beam source in a vacuum chamber intermittently by a shutter mechanism to grow a semiconductor crystal film on the semiconductor substrate, the shutter is bent. A molecular beam source characterized in that the open end is rotated about a rotation axis other than the central axis of one open end, and the open end is opposed to the molecular beam injection port of the crucible.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13998289A JPH034516A (en) | 1989-06-01 | 1989-06-01 | Molecular beam source |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13998289A JPH034516A (en) | 1989-06-01 | 1989-06-01 | Molecular beam source |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH034516A true JPH034516A (en) | 1991-01-10 |
Family
ID=15258190
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP13998289A Pending JPH034516A (en) | 1989-06-01 | 1989-06-01 | Molecular beam source |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH034516A (en) |
-
1989
- 1989-06-01 JP JP13998289A patent/JPH034516A/en active Pending
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