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JPS6136371B2 - - Google Patents
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JPS6136371B2 - - Google Patents

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Publication number
JPS6136371B2
JPS6136371B2 JP2190978A JP2190978A JPS6136371B2 JP S6136371 B2 JPS6136371 B2 JP S6136371B2 JP 2190978 A JP2190978 A JP 2190978A JP 2190978 A JP2190978 A JP 2190978A JP S6136371 B2 JPS6136371 B2 JP S6136371B2
Authority
JP
Japan
Prior art keywords
gas
reaction gas
injected
epitaxial growth
epitaxially grown
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
JP2190978A
Other languages
Japanese (ja)
Other versions
JPS54114178A (en
Inventor
Junji Sakurai
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP2190978A priority Critical patent/JPS54114178A/en
Publication of JPS54114178A publication Critical patent/JPS54114178A/en
Publication of JPS6136371B2 publication Critical patent/JPS6136371B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】[Detailed description of the invention]

本発明は、シリコンのような半導体の特に薄い
膜を高精度の比抵抗を有するように再現性良く成
長させるのに好適な真空エピタキシヤル成長方法
に関する。 従来、例えば化学気相成長法(CVD法)に依
りシリコン膜を形成するには、モノ・シラン
(SiH4)或いはハロゲン化シリコン(SiCl4
SiH2Cl3等)をを水素(H2)や不活性ガス等のキ
ヤリヤ・ガスに依つてシリコン半導体基板表面に
輸送し、そこで熱分解させることに依りエピタキ
シヤル成長させている。従つて、エピタキシヤル
成長膜の厚さは前記反応ガスとキヤリヤ・ガスと
の混合ガスの流れ方に大きく依存し、同一ウエハ
内、同一反応装置内に於いても場所に依存する厚
さの分布を生じ易く、また、ロツト間の不均一も
大きくなり勝ちである。しかも、シリコン・エピ
タキシヤル成長膜中に燐(P+)、硼素(B+)等の
不純物原子を1014〜1017〔cm-3〕程度に薄くドー
ピングすることを再現性良く実施することは現在
のところ不可能に近い。これは、反応装置内で前
記混合ガスの均一な流れが得難く、特に、シリコ
ン半導体基板表面では、吸気と排気の関係から、
或る場所では層流に、或る場所では乱流になつた
り、また、熱分解を起した残りのガス成分がシリ
コン半導体基板表面に停滞し、新しい未反応のガ
スが該表面に到達することを妨げたりする為であ
る。尚、近年、前記CVD法とは別に分子線エピ
タキシヤル成長法の開発が盛んであるが、この方
法を実施するには大規模の装置が必要であり、例
えば、成長速度の制御は蒸着ルツボの温度を制御
することに依り行なうが、それには電子計算機を
用いなければならず、また、その制御にも多くの
困難があり、未だ量産プロセスへの適用はでき
ず、実験的段階を出ていない。 本発明は、CVD法と分子線エピタキシヤル成
長法それぞれの特徴を兼ね備えるエピタキシヤル
成長方法を提供し、高精度に制御された比抵抗を
有する半導体エピタキシヤル成長膜を再現性良く
量産できるようにするものであり、以下これを詳
細に説明する。 図は本発明を実施するのに用いる装置の一例を
表わす要部側断面図である。 図に於いて、1はベル・ジヤー、1aはガス噴
射口、2は底板、2aはガス排出口、3はサスセ
プタ、4はシリコン・ウエハをそれぞれ示す。 本装置を用いて本発明を実施する場合の一例を
説明する。 即ち、サスセプタ3上にウエハ4をセツトす
る。それ等は900〜1000〔℃〕の温度に加熱でき
るようになつている。ベル・ジヤー1内は1×
10-3〔Torr〕以下に排気する。噴射口1aはサ
スセプタ3上にセツトされたウエハ4の全てを見
込む位置に形成され、そこからは混合ガスが一定
量ずつ断続的に噴射される。混合ガスは場合に依
つては反応ガス単独に代えても良い。このように
すると、一定量のガスは、噴射口1aから直線的
にウエハ4に到達し、その表面で分解し、一定の
厚さのエピタキシヤル成長膜が形成される。そし
て、次の噴射ガスが到達するまでには、その前に
分解したガスは全て排気され、完全に当初の状態
に戻つている。エピタキシヤル成長膜に不純物を
含有させたい場合には、噴射ガスにドーパント・
ガス(例えばPCl3,B2H6等)を混合すれば良
い。 前記実施例に於いて、1回のガス噴射に依り、
厚さがどれだけのエピタキシヤル成長膜を形成で
きるのかは、噴射ガスに於ける反応ガスの濃度、
噴射量に依つて決められ、しかも、それ等は広範
囲に亘つて精度良く変化させることが可能である
から、所望膜厚のエピタキシヤル成長膜を得るに
は所定ガスを用いて何回の噴射をすれば良いか予
め正確に知ることができ、また、実施することが
できる。そして、間欠的に噴射されるガスの間に
は何等の相互干渉もないので、エピタキシヤル成
長はミクロ的に見ても同一条件で行なわれ、従つ
て、再現性が非常に良い。また、薄い不純物ドー
ピングをしたい場合も同様であつて、ドーバン
ド・ガス分子が直接シリコン・ウエハ4の表面に
衝突して、常に同一の確率で反応を起すようにす
ることができるから、分布、再現性ともに優れた
ライト・ドーブド・エピタキシヤル(light
dopedepitaxial)成長膜を形成することが可能で
ある。 次に、具体例を数値に依つて説明しよう。 1 図のベル・ジヤー1として容積約50〔〕の
ものを用い、内部を1×10-4〔Torr〕以下に
保ち、100〔%〕モノ・シランを約4〔ml〕(1
〔Torr〕、常温)ずつ1〔秒〕間隔で100〔回〕
噴射した。このときサスセプタ3上のシリコ
ン・ウエハ4の温度は950〔℃〕に維持した。
1〔回〕の噴射で50〔Å〕のエピタキシヤル成
長膜が得られるので最終的には5000〔Å〕の膜
厚になつた。この場合の膜厚分布は、 ロツト内(7.5〔cm〕φ即ち3〔イワチ〕φ
ウエハを5〔枚〕):5000〔Å〕±20〔Å〕 ロツト間(10〔回〕の平均):5000〔Å〕±
50〔Å〕であつた。 2 前記1と同様に反応装置をセツトし、噴射ガ
スとして100〔%〕モノ・シランに100
〔ppm〕ジボランを1:10-3の比でベル・ジヤ
ー1の直前で均一に混合し、また、ジボランが
重合したり装置壁面で分解するのを防止する
為、混合ガスを約10〔℃〕以下に冷却する等の
操作を加え、そして、前記1と同様にして前記
混合ガスを噴射してエピタキシヤル成長を行な
つた。それに依り、比抵抗0.1〔Ω・cm〕のn+
型シリコン・ウエハ上に5000〔Å〕±20〔Å〕
のp-(比抵抗10±1〔Ω・cm〕)のエピタキシ
ヤル成長膜が再現性良く得られた。 以上説明した本発明に依る効果を列挙すると次
の通りである。 (イ) 従来の気相エピタキシヤル成長方法に比較す
ると、ウエハ内は勿論、ロツト内或いはロツト
間であつてもエピタキシヤル成長膜の膜厚分布
は極めて少なく、また、分子線エピタキシヤル
成長方法に比較すると、実施する際に必要とさ
れる装置は著しく簡単であり、気相エピタキシ
ヤル成長方法の実施に用いる装置にガスを間欠
噴射する装置を付加したり、ガス噴射口の位置
を適宜に選定するだけで実用になり、後は装置
の比較的簡単な制御を行なえば良い。 (ロ) 不純物ドーピングを広範囲に変え、所望の比
抵抗を有するエピタキシヤル層を安定して成長
させることができる。 (ハ) 分子線エピタキシヤル成長方法を適用しない
と得られないような薄い膜厚のエピタキシヤル
成長膜を高精度で再現性良く得られる。 (ニ) 分子線エピタキシヤル成長方法とは全く比較
にならない程、多量のウエハを同時に短時間で
処理できる。 (ホ) エピタキシヤル成長は短時間で、しかも、稀
薄なガス雰囲気の下で行なわれるので、ウエハ
からエピタキシヤル成長膜に対するオート・ド
ーピングや不純物の這い上りは著しく減少す
る。 (ヘ) 従来の気相エピタキシヤル成長方法と比較す
ると、結晶欠陥や凹凸等が少ない良質のエピタ
キシヤル成長膜が得られる。 このように、本発明に依ると従来の気相成長方
法や分子線エピタキシヤル成長方法と比較すると
種々の優れた効果を有しているが、他の特徴とす
るところを集約比較すると次表の通りである。
The present invention relates to a vacuum epitaxial growth method suitable for growing a particularly thin film of a semiconductor such as silicon with high reproducibility so as to have a highly precise resistivity. Conventionally, to form a silicon film by chemical vapor deposition (CVD), for example, monosilane (SiH 4 ) or silicon halide (SiCl 4 ,
Epitaxial growth is achieved by transporting SiH 2 Cl 3 (SiH 2 Cl 3 etc.) to the surface of a silicon semiconductor substrate using a carrier gas such as hydrogen (H 2 ) or an inert gas, and thermally decomposing it there. Therefore, the thickness of the epitaxially grown film largely depends on the flow of the mixed gas of the reaction gas and carrier gas, and the thickness distribution varies depending on the location even within the same wafer or within the same reaction device. In addition, the non-uniformity between lots tends to increase. Moreover, it is difficult to dope impurity atoms such as phosphorus (P + ) and boron (B + ) in a thin layer of 10 14 to 10 17 [cm -3 ] with good reproducibility in a silicon epitaxially grown film. It's close to impossible at the moment. This is because it is difficult to obtain a uniform flow of the mixed gas within the reactor, and especially on the silicon semiconductor substrate surface, due to the relationship between intake and exhaust.
The flow becomes laminar in some places and turbulent in others, and the remaining gas components that have undergone thermal decomposition stagnate on the surface of the silicon semiconductor substrate, and new unreacted gases reach the surface. This is to prevent the In addition, in recent years, development of molecular beam epitaxial growth methods apart from the above-mentioned CVD method has been active, but implementing this method requires large-scale equipment. For example, controlling the growth rate requires the use of a deposition crucible. This is done by controlling the temperature, but this requires the use of an electronic computer, and there are many difficulties in controlling it, so it has not yet been able to be applied to mass production processes and has not moved beyond the experimental stage. . The present invention provides an epitaxial growth method that combines the characteristics of the CVD method and the molecular beam epitaxial growth method, and makes it possible to mass-produce semiconductor epitaxially grown films with highly precisely controlled resistivity with good reproducibility. This will be explained in detail below. The figure is a side sectional view of a main part showing an example of a device used to carry out the present invention. In the figure, 1 is a bell jar, 1a is a gas injection port, 2 is a bottom plate, 2a is a gas discharge port, 3 is a susceptor, and 4 is a silicon wafer. An example of implementing the present invention using this device will be described. That is, the wafer 4 is set on the susceptor 3. They can be heated to temperatures of 900 to 1000 degrees Celsius. Inside Bell Jar 1 is 1x
Exhaust to below 10 -3 [Torr]. The injection port 1a is formed at a position where it can see all of the wafers 4 set on the susceptor 3, and a fixed amount of the mixed gas is intermittently injected from there. Depending on the case, the mixed gas may be replaced with the reactive gas alone. In this way, a certain amount of gas linearly reaches the wafer 4 from the injection port 1a, decomposes on the surface of the wafer 4, and forms an epitaxially grown film of a certain thickness. By the time the next injection gas arrives, all the previously decomposed gas has been exhausted and the system has completely returned to its original state. If you want to include impurities in the epitaxially grown film, add a dopant to the injection gas.
It is sufficient to mix gases (for example, PCl 3 , B 2 H 6, etc.). In the above embodiment, by one gas injection,
The thickness of the epitaxially grown film that can be formed depends on the concentration of the reactant gas in the injection gas,
It is determined by the injection amount, and since it is possible to vary it over a wide range with high precision, it is important to know how many injections are required using a specified gas in order to obtain an epitaxially grown film of the desired thickness. You can know in advance exactly what you need to do, and you can also implement it. Since there is no mutual interference between the intermittently injected gases, epitaxial growth is performed under the same conditions even from a microscopic point of view, and therefore the reproducibility is very good. The same is true when thin impurity doping is desired; the doped gas molecules directly collide with the surface of the silicon wafer 4, and the reaction always occurs with the same probability. Light doped epitaxial with excellent properties.
It is possible to form a dopedepitaxial) growth film. Next, let's explain a concrete example using numerical values. 1 Use a bell jar 1 with a volume of about 50 [] as shown in the figure, keep the inside at 1 × 10 -4 [Torr] or less, and add about 4 [ml] (1
[Torr], room temperature) 100 times at 1 [second] intervals
It was injected. At this time, the temperature of the silicon wafer 4 on the susceptor 3 was maintained at 950 [°C].
Since an epitaxially grown film of 50 [Å] was obtained with one injection, the final film thickness was 5000 [Å]. In this case, the film thickness distribution is within the lot (7.5 [cm] φ or 3 [Iwachi] φ
5 [wafers]): 5000 [Å] ± 20 [Å] Between lots (average of 10 [wafers]): 5000 [Å] ±
It was 50 [Å]. 2 Set up the reaction apparatus in the same manner as in 1 above, and add 100% monosilane to 100% as the injection gas.
[ppm] Diborane was mixed uniformly in a ratio of 1:10 -3 just before bell jar 1, and the mixed gas was heated at about 10 [℃] to prevent diborane from polymerizing or decomposing on the walls of the equipment. ] The following operations such as cooling were added, and the mixed gas was injected in the same manner as in 1 above to perform epitaxial growth. Accordingly, n + of specific resistance 0.1 [Ω・cm]
5000〔Å〕±20〔Å〕 on mold silicon wafer
An epitaxially grown film with a p - (specific resistance of 10±1 [Ω·cm]) was obtained with good reproducibility. The effects of the present invention explained above are listed below. (b) Compared to the conventional vapor phase epitaxial growth method, the thickness distribution of the epitaxially grown film is extremely small not only within the wafer but also within a lot or between lots; In comparison, the equipment required to carry out the method is significantly simpler; it is possible to add a device for intermittently injecting gas to the equipment used to carry out the vapor phase epitaxial growth method, or to select the position of the gas injection port appropriately. It can be put into practical use just by doing this, and then all you have to do is perform relatively simple control of the device. (b) It is possible to stably grow an epitaxial layer having a desired resistivity by changing impurity doping over a wide range. (c) It is possible to obtain thin epitaxially grown films with high precision and good reproducibility, which cannot be obtained without applying the molecular beam epitaxial growth method. (d) A large number of wafers can be processed simultaneously in a short time, which is completely incomparable to the molecular beam epitaxial growth method. (e) Since epitaxial growth is carried out in a short time and in a dilute gas atmosphere, auto-doping and impurity creep-up from the wafer to the epitaxially grown film are significantly reduced. (F) Compared with conventional vapor phase epitaxial growth methods, a high quality epitaxially grown film with fewer crystal defects, irregularities, etc. can be obtained. As described above, the present invention has various superior effects compared to conventional vapor phase growth methods and molecular beam epitaxial growth methods, but when compared with other characteristics, the following table shows the following. That's right.

【表】【table】

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

図は本発明を実施する装置の一例を表わす要部
側断面図である。 図に於いて、1はベル・ジヤー、1aはガス噴
射口、2は底板、2aはガス排出口、3はサスセ
プタ、4はシリコン・ウエハをそれぞれ示す。
The figure is a side cross-sectional view of essential parts showing an example of an apparatus for carrying out the present invention. In the figure, 1 is a bell jar, 1a is a gas injection port, 2 is a bottom plate, 2a is a gas discharge port, 3 is a susceptor, and 4 is a silicon wafer.

Claims (1)

【特許請求の範囲】 1 サスセプタ上に半導体ウエハが載置された反
応装置内を所定気圧を維持するように排気を行
い、 次いで、前記半導体ウエハを見込む位置に在る
ガス噴射口から反応ガスを噴射して前記半導体ウ
エハ表面に直接到達せしめ熱分解を行つて半導体
膜をエピタキシヤル成長させ、 次いで、前記反応装置内が前記反応ガスの噴射
前に於ける前記所定気圧を維持するように排気さ
れた時点で前記と同様に反応ガスの噴射及び該反
応ガスの熱分解を行つて半導体膜をエピタキシヤ
ル成長させ、 必要に応じ前記排気完了後に於ける反応ガスの
噴射及び反応ガスの熱分解の工程を繰り返すこと
に依り所定膜厚の半導体膜を複数回に分けてエピ
タキシヤル成長させること を特徴とする真空エピタキシヤル成長方法。
[Claims] 1. Evacuate the inside of a reaction device in which a semiconductor wafer is placed on a susceptor to maintain a predetermined atmospheric pressure, and then inject a reaction gas from a gas injection port located at a position facing the semiconductor wafer. The reactant gas is injected to directly reach the surface of the semiconductor wafer and thermally decomposed to epitaxially grow a semiconductor film, and then the inside of the reactor is evacuated to maintain the predetermined pressure before the reaction gas is injected. At that point, the reaction gas is injected and the reaction gas is thermally decomposed in the same manner as above to epitaxially grow the semiconductor film, and if necessary, the reaction gas injection and reaction gas thermal decomposition steps are carried out after the evacuation is completed. A vacuum epitaxial growth method characterized in that a semiconductor film of a predetermined thickness is epitaxially grown in multiple steps by repeating the steps.
JP2190978A 1978-02-27 1978-02-27 Vacuum epitaxial growing method Granted JPS54114178A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2190978A JPS54114178A (en) 1978-02-27 1978-02-27 Vacuum epitaxial growing method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2190978A JPS54114178A (en) 1978-02-27 1978-02-27 Vacuum epitaxial growing method

Publications (2)

Publication Number Publication Date
JPS54114178A JPS54114178A (en) 1979-09-06
JPS6136371B2 true JPS6136371B2 (en) 1986-08-18

Family

ID=12068211

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2190978A Granted JPS54114178A (en) 1978-02-27 1978-02-27 Vacuum epitaxial growing method

Country Status (1)

Country Link
JP (1) JPS54114178A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57173933A (en) * 1981-04-17 1982-10-26 Nippon Telegr & Teleph Corp <Ntt> Growing method for molecular beam
JPS63152118A (en) * 1986-12-16 1988-06-24 Fujitsu Ltd Manufacture of semiconductor device
JP4719478B2 (en) * 2005-02-09 2011-07-06 学校法人東京理科大学 Granule injection device

Also Published As

Publication number Publication date
JPS54114178A (en) 1979-09-06

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