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JPS6231814B2 - - Google Patents
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JPS6231814B2 - - Google Patents

Info

Publication number
JPS6231814B2
JPS6231814B2 JP55140444A JP14044480A JPS6231814B2 JP S6231814 B2 JPS6231814 B2 JP S6231814B2 JP 55140444 A JP55140444 A JP 55140444A JP 14044480 A JP14044480 A JP 14044480A JP S6231814 B2 JPS6231814 B2 JP S6231814B2
Authority
JP
Japan
Prior art keywords
diffusion
gallium
tube
temperature
container
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
JP55140444A
Other languages
Japanese (ja)
Other versions
JPS5764923A (en
Inventor
Osamu Saito
Hideo Pponma
Koichi Inoe
Naohiro Monma
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP55140444A priority Critical patent/JPS5764923A/en
Priority to US06/291,042 priority patent/US4415385A/en
Publication of JPS5764923A publication Critical patent/JPS5764923A/en
Publication of JPS6231814B2 publication Critical patent/JPS6231814B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10PGENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
    • H10P32/00Diffusion of dopants within, into or out of wafers, substrates or parts of devices

Landscapes

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

Description

【発明の詳細な説明】 本発明は、半導体基体へのガリウム拡散法に係
り、特に元素状ガリウムを拡散不純物として、半
導体基体中にガリウムを熱拡散する半導体へのガ
リウム拡散法に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for diffusing gallium into a semiconductor substrate, and more particularly to a method for diffusing gallium into a semiconductor substrate by thermally diffusing gallium into a semiconductor substrate using elemental gallium as a diffusion impurity.

半導体基体中にp型不純物領域を形成するため
の不純物としてホウ素が広く用いられている。し
かし、ホウ素は半導体基体中での拡散速度が著し
く遅いので、深い接合を形成するのに長い時間が
かかり、コストの点で大変不利となつている。
Boron is widely used as an impurity for forming p-type impurity regions in semiconductor substrates. However, since boron has an extremely slow diffusion rate in a semiconductor substrate, it takes a long time to form a deep junction, which is very disadvantageous in terms of cost.

そこで、深い接合の形成には半導体基体中での
拡散速度の速いガリウムが用いられる。特に高耐
圧で高ライフタイムの接合を形成するためには、
ガリウム供給源は、高純度のものであることが必
要で、この点、元素状ガリウムは十分満足できる
拡散源である。ところが、元素状ガリウムは低温
で著しく蒸気圧が低く、かつ酸化しやすいという
性質があるため、所望の不純物量を、しかも均一
に拡散することは困難であつた。そこで、元素状
ガリウムを拡散不純物源とする場合、不純物源と
半導体基体とを酸素を含まない高温均熱領域に閉
じ込めなければならない。このような事情から、
従来、元素状ガリウムを不純物源としたガリウム
拡散は、閉管法という方法で行なわれていた。こ
の方法では、拡散不純物源を半導体基体ととも
に、石英拡散管の中に置き、管内を真空あるい
は、不活性ガスで充填し、石英拡散管を溶封した
後、拡散熱処理する。しかしこの場合、拡散後、
半導体基体を取り出すため、石英管を切断しなけ
ればならないため、石英拡散管は再使用ができ
ず、きわめて不経済である。
Therefore, gallium, which has a high diffusion rate in the semiconductor substrate, is used to form deep junctions. In particular, in order to form a bond with high voltage resistance and long lifetime,
The gallium source must be of high purity, and elemental gallium is a satisfactory diffusion source in this respect. However, since elemental gallium has a significantly low vapor pressure at low temperatures and is easily oxidized, it has been difficult to uniformly diffuse a desired amount of impurities. Therefore, when elemental gallium is used as a diffused impurity source, the impurity source and the semiconductor substrate must be confined in a high-temperature soaking region that does not contain oxygen. Due to these circumstances,
Conventionally, gallium diffusion using elemental gallium as an impurity source has been carried out by a closed tube method. In this method, a diffusion impurity source and a semiconductor substrate are placed in a quartz diffusion tube, the tube is vacuumed or filled with an inert gas, the quartz diffusion tube is melt-sealed, and then diffusion heat treatment is performed. However, in this case, after diffusion,
Since the quartz tube must be cut to remove the semiconductor substrate, the quartz diffusion tube cannot be reused and is extremely uneconomical.

そこで、この問題点を解消するため、真空開管
法という方法が提案されている。この方法は、拡
散不純物源と半導体基体を拡散管の中にいれ、管
内を真空排気装置で排気しながら真空状態を保
ち、そのまま拡散管の中の不純物源と半導体基体
を高温均熱領域に入れ拡散熱処理するものであ
る。この真空開管法は、拡散管を溶封しないた
め、閉管法の問題点は解消する。しかし、実際の
拡散への適用にあたつては、拡散管の材質が問題
となる。拡散管の材質としては、現時点では純度
の点で石英が好適であるが、石英は、ガリウム蒸
気と反応するため、石英の拡散管は強度的に弱く
なり破損しやすいという問題がある。特に大気圧
以下の減圧状態では、石英拡散管には強い力がか
かるため、管自体の寿命もきわめて短かくなる。
In order to solve this problem, a method called the vacuum open tube method has been proposed. In this method, a diffused impurity source and a semiconductor substrate are placed in a diffusion tube, the inside of the tube is evacuated using a vacuum evacuation device to maintain a vacuum state, and the impurity source and semiconductor substrate inside the diffusion tube are placed in a high-temperature soaking area. Diffusion heat treatment is applied. This vacuum open tube method eliminates the problems of the closed tube method because the diffusion tube is not melt-sealed. However, in actual application to diffusion, the material of the diffusion tube becomes a problem. Currently, quartz is preferred as a material for the diffusion tube in terms of purity, but since quartz reacts with gallium vapor, there is a problem that quartz diffusion tubes become weak in strength and easily break. Particularly in a reduced pressure state below atmospheric pressure, a strong force is applied to the quartz diffusion tube, and the life of the tube itself is extremely shortened.

それゆえ本発明の目的は、所望の不純物量を均
一性良く拡散することができる半導体基体へのガ
リウム拡散法を提供することにある。
Therefore, an object of the present invention is to provide a method for diffusing gallium into a semiconductor substrate, which allows a desired amount of impurities to be diffused with good uniformity.

また、本発明の他の目的は石英を拡散管として
用いた場合、その寿命が長い半導体基体へのガリ
ウム拡散法を提供することにある。
Another object of the present invention is to provide a method for diffusing gallium into a semiconductor substrate that has a long life when quartz is used as a diffusion tube.

本発明の特徴とするところは、半導体基体を元
素状ガリウムとともに半封じ状態の容器にいれ、
その容器をガス圧調整ができる拡散管の中に挿入
し、不活性ガスで管内をガス置換し所定のガス圧
状態にして、拡散熱処理することにある。
The present invention is characterized by placing a semiconductor substrate together with elemental gallium in a semi-closed container,
The container is inserted into a diffusion tube whose gas pressure can be adjusted, and the inside of the tube is replaced with an inert gas to achieve a predetermined gas pressure, and diffusion heat treatment is performed.

半封じ状態の容器の開口面積は、容器の断面積
の2〜10%がよい。また、拡散管内における不活
性ガスのガス圧としては10Torr〜大気圧がよ
い。
The opening area of a semi-closed container is preferably 2 to 10% of the cross-sectional area of the container. Further, the gas pressure of the inert gas in the diffusion tube is preferably 10 Torr to atmospheric pressure.

以下、本発明を図面に基づいて説明する。 Hereinafter, the present invention will be explained based on the drawings.

第1図は本発明の一実施例を示している。 FIG. 1 shows an embodiment of the invention.

第1図に示すように、片側を閉じた外径65mm、
内径61mm、長さ500mmの石英容器1中に拡散不純
物源として50mgの元素状ガリウム2をいれたシリ
コンボート3、半導体基体として石英ウエハホル
ダー4にたてた直径50mm、厚さ500μm、20枚の
シリコンウエハ5、50mgの元素状ガリウム2をい
れたシリコンボート3の順に配置し、さらに外径
60mmの石英内栓6で蓋をした。この石英容器1
を、第1図の石英拡散管7内に開閉口8から挿入
した後、真空排気装置9と不活性ガスとしてN2
ガスを用いたガス供給装置10により、ガス置換
し管内の雰囲気をN2ガス雰囲気とした後排気す
るという操作を3回繰返した。そして10-6Torr
の圧力で連続排気しながら加熱用ヒータ11によ
り600℃まで温度をあげ、10分間温度保持した後
N2ガスを徐々に充填し、管内を大気圧にしたう
えで10分間600℃で温度保持した。この状態から
温度を1150℃の拡散温度まであげ3時間の温度保
持の後冷却し600℃で容器1を拡散管7からとり
だした。
As shown in Figure 1, the outer diameter is 65 mm with one side closed.
A silicon boat 3 containing 50 mg of elemental gallium 2 as a diffused impurity source is placed in a quartz container 1 with an inner diameter of 61 mm and a length of 500 mm, and a silicon boat 3 with a diameter of 50 mm and a thickness of 500 μm and 20 wafers placed on a quartz wafer holder 4 as a semiconductor substrate. Silicon wafer 5, silicon boat 3 containing 50 mg of elemental gallium 2 are placed in this order, and the outer diameter
It was capped with a 60 mm quartz inner stopper 6. This quartz container 1
is inserted into the quartz diffusion tube 7 shown in FIG.
Using the gas supply device 10 using gas, the operation of replacing the gas and changing the atmosphere inside the tube to an N 2 gas atmosphere and then exhausting the tube was repeated three times. and 10 -6 Torr
The temperature was raised to 600℃ using the heating heater 11 while continuously exhausting at a pressure of
N 2 gas was gradually filled to bring the inside of the tube to atmospheric pressure, and the temperature was maintained at 600°C for 10 minutes. From this state, the temperature was increased to a diffusion temperature of 1150°C, maintained at the temperature for 3 hours, and then cooled, and the container 1 was taken out from the diffusion tube 7 at 600°C.

第2図は容器1の開口率と拡散後のシリコンウ
エハ5におけるシート抵抗の関係を示している。
FIG. 2 shows the relationship between the aperture ratio of the container 1 and the sheet resistance of the silicon wafer 5 after diffusion.

ここで、開口率とは容器1の断面積に対する半
封じ状態の容器1の開口面積の割合を%表示した
ものである。
Here, the opening ratio is the ratio of the opening area of the semi-closed container 1 to the cross-sectional area of the container 1, expressed as a percentage.

開口率が10%より大きいと、ガリウム蒸気を閉
じ込める効果が少なくなり、また2%より小さい
と逆に容器内のガス置換、圧力調整が難かしく、
拡散不純物源の酸化の原因となり、拡散層の不純
物量の目安となるシート抵抗は所望の値ρSOとな
らない。
If the opening ratio is larger than 10%, the effect of trapping gallium vapor will be reduced, and if it is smaller than 2%, it will be difficult to replace the gas inside the container and adjust the pressure.
This causes oxidation of the diffused impurity source, and the sheet resistance, which is a measure of the amount of impurities in the diffused layer, does not reach the desired value ρ SO .

このような半封じ状態において、拡散熱処理時
の不活性ガス圧は、少なくとも10Torr〜大気圧
でなければならない。というのは、10Torr以下
のガス圧の場合、開口部でのガリウム蒸気の流通
が良く、容器1内のガリウム蒸気が容器1外にと
びだし外の拡散管7と反応し、容器1内の蒸気圧
が十分高くならず第3図に示すように、拡散後の
シリコンウエハのシート抵抗は高く所望の値ρSO
とならないためである。また10Torr以上のガス
圧の場合は、開口部での蒸気の流通が悪くなり、
容器1内の蒸気圧が十分高くなり所望のシート抵
抗値を均一性良く得ることができる。
In such a semi-sealed state, the inert gas pressure during the diffusion heat treatment must be at least 10 Torr to atmospheric pressure. This is because when the gas pressure is 10 Torr or less, the gallium vapor flows well at the opening, and the gallium vapor inside the container 1 flows out of the container 1 and reacts with the diffusion tube 7 outside, causing the vapor pressure inside the container 1 to decrease. is not high enough, and as shown in Figure 3, the sheet resistance of the silicon wafer after diffusion is high enough to reach the desired value ρ SO
This is to prevent this from happening. In addition, if the gas pressure is over 10 Torr, the flow of steam at the opening will be poor.
The vapor pressure within the container 1 becomes sufficiently high, and a desired sheet resistance value can be obtained with good uniformity.

尚、上記の開口率、不活性ガス圧は、所望のシ
ート抵抗を変えても、同様に適用できる数値であ
る。
Note that the above aperture ratio and inert gas pressure are numerical values that can be similarly applied even if the desired sheet resistance is changed.

それは、容器からガリウム蒸気がとびだす条件
は変わらないからである。
This is because the conditions under which gallium vapor escapes from the container remain the same.

また拡散工程は、第4図の手順で行なうことが
望ましい。室温において、不活性ガスで数回バツ
クフイルと排気を繰返す理由は、容器内1の残留
酸素を少しでも少なくし、不純物源の酸化を防止
するためである。また、拡散熱処理時の拡散温度
より低い温度での低温(500〜800℃)の熱処理
は、連続排気の真空状態とし、一種の空焼きの効
果をもたせて、拡散温度での系内の不用な不純物
の影響をさけるためのものである。
Further, it is desirable that the diffusion process be performed in accordance with the procedure shown in FIG. The reason why backfilling and evacuation are repeated several times with an inert gas at room temperature is to reduce the amount of residual oxygen in the container 1 as much as possible and prevent oxidation of the impurity source. In addition, the low-temperature (500 to 800°C) heat treatment at a temperature lower than the diffusion temperature during diffusion heat treatment is performed in a continuous evacuation vacuum state, which creates a kind of dry firing effect and eliminates waste in the system at the diffusion temperature. This is to avoid the influence of impurities.

すなわち、室温から拡散温度まで、比較的低い
真空度もしくは大気圧の不活性ガス雰囲気で熱処
理しているが、この間に、容器1内の残留酸素及
び容器1内に吸着されている酸素や水分が温度上
昇に伴つて放出され、元素状ガリウムが酸化され
その結果、シート抵抗の均一性が悪くなる。そこ
で、放出された酸素や水分を十分に除去し、シー
ト抵抗の均一性をより向上させるため、拡散管内
を連続排気しつつ、低温熱処理を行うのである。
That is, the heat treatment is performed from room temperature to the diffusion temperature in an inert gas atmosphere at a relatively low degree of vacuum or atmospheric pressure, but during this time, residual oxygen in the container 1 and oxygen and moisture adsorbed in the container 1 are As the temperature rises, it is released and elemental gallium is oxidized, resulting in poor sheet resistance uniformity. Therefore, in order to sufficiently remove the released oxygen and moisture and further improve the uniformity of sheet resistance, low-temperature heat treatment is performed while the interior of the diffusion tube is continuously evacuated.

因みに、低温熱処理を行なわない場合における
シート抵抗のばらつきは±10%程度あつた。
Incidentally, the variation in sheet resistance when low-temperature heat treatment was not performed was approximately ±10%.

以上説明したように、本発明によれば、ガリウ
ムを半導体基体に均一に、しかも所望の値に拡散
することができる。測定結果によれば拡散層のシ
ート抵抗のばらつきは同一ロツド内で±3%以下
であつた。
As described above, according to the present invention, gallium can be uniformly diffused into a semiconductor substrate to a desired value. According to the measurement results, the variation in sheet resistance of the diffusion layer was within ±3% within the same rod.

また、本発明によれば、容器1、拡散管の寿命
は長く、10回以上、繰り返し使用することができ
た。
Furthermore, according to the present invention, the container 1 and the diffusion tube had a long lifespan and could be used repeatedly more than 10 times.

因みに、従来法によれば、3〜4回で拡散管を
交換しなければならなかつた。
Incidentally, according to the conventional method, the diffusion tube had to be replaced every 3 to 4 times.

なお、本発明においては上例にかぎらず半導体
基体としてゲルマニウム等を用いることは可能で
あり、容器としてタンタル等を用いても同様の効
果が得られる。
Note that the present invention is not limited to the above example, and it is possible to use germanium or the like as the semiconductor substrate, and the same effect can be obtained even if tantalum or the like is used as the container.

また、不活性ガスとしてアルゴンガス等を用い
ても、同様の効果が得られる。
Furthermore, similar effects can be obtained by using argon gas or the like as the inert gas.

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

第1図は本発明の一実施例を示す拡散炉の断面
図、第2図は本発明において拡散のために用いら
れる容器の開口率とシリコンウエハにおける拡散
層のシート抵抗の関係を示す図、第3図は同じく
拡散管内の圧力とシリコンウエハにおける拡散層
のシート抵抗の関係を示す図、第4図は本発明の
実施に好適な拡散プログラムを示す図である。 1…容器、2…元素状ガリウム、3…シリコン
ボート、4…石英ウエハホルダー、5…シリコン
ウエハ、6…石英内栓、7…石英拡散管、8…開
閉口、9…真空排気装置、10…不活性ガス供給
装置、11…加熱用ヒータ。
FIG. 1 is a cross-sectional view of a diffusion furnace showing an embodiment of the present invention, and FIG. 2 is a diagram showing the relationship between the aperture ratio of a container used for diffusion in the present invention and the sheet resistance of a diffusion layer in a silicon wafer. FIG. 3 is a diagram showing the relationship between the pressure inside the diffusion tube and the sheet resistance of the diffusion layer in the silicon wafer, and FIG. 4 is a diagram showing a diffusion program suitable for implementing the present invention. DESCRIPTION OF SYMBOLS 1... Container, 2... Elemental gallium, 3... Silicon boat, 4... Quartz wafer holder, 5... Silicon wafer, 6... Quartz inner plug, 7... Quartz diffusion tube, 8... Opening/closing port, 9... Vacuum exhaust device, 10 ...Inert gas supply device, 11...Heating heater.

Claims (1)

【特許請求の範囲】 1 元素状ガリウムを拡散不純物源として半導体
基板とともに断面積に対する開口面積の割合が2
〜10%である反応容器内に配置し、 前記反応容器をガス圧調整可能な石英拡散管内
に配置し、 500〜800℃の温度で熱処理を行なつて前記反応
容器内に吸着されている酸素あるいは水分を除去
し、 前記石英拡散管内に不活性ガスを10Torr〜大
気圧に充填し、 前記反応容器をさらに昇温させてガリウムの拡
散温度に保持し、 その後、前記反応容器を冷却する ことを特徴とする半導体基体へのガリウム拡散
法。
[Claims] 1. Elemental gallium is used as a diffused impurity source and the ratio of the opening area to the cross-sectional area is 2 along with the semiconductor substrate.
~10% in a reaction vessel, the reaction vessel is placed in a quartz diffusion tube where the gas pressure can be adjusted, and heat treatment is performed at a temperature of 500 to 800°C to remove the oxygen adsorbed in the reaction vessel. Alternatively, remove moisture, fill the quartz diffusion tube with an inert gas at a pressure of 10 Torr to atmospheric pressure, further raise the temperature of the reaction vessel to maintain it at the gallium diffusion temperature, and then cool the reaction vessel. Characteristic method of gallium diffusion into semiconductor substrates.
JP55140444A 1980-08-15 1980-10-09 Method for diffusing gallium in semiconductor substrate Granted JPS5764923A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP55140444A JPS5764923A (en) 1980-10-09 1980-10-09 Method for diffusing gallium in semiconductor substrate
US06/291,042 US4415385A (en) 1980-08-15 1981-08-07 Diffusion of impurities into semiconductor using semi-closed inner diffusion vessel

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP55140444A JPS5764923A (en) 1980-10-09 1980-10-09 Method for diffusing gallium in semiconductor substrate

Publications (2)

Publication Number Publication Date
JPS5764923A JPS5764923A (en) 1982-04-20
JPS6231814B2 true JPS6231814B2 (en) 1987-07-10

Family

ID=15268771

Family Applications (1)

Application Number Title Priority Date Filing Date
JP55140444A Granted JPS5764923A (en) 1980-08-15 1980-10-09 Method for diffusing gallium in semiconductor substrate

Country Status (1)

Country Link
JP (1) JPS5764923A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2662318B2 (en) * 1991-03-13 1997-10-08 株式会社日立製作所 Method of diffusing impurities into semiconductor substrate

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5028752A (en) * 1973-07-13 1975-03-24

Also Published As

Publication number Publication date
JPS5764923A (en) 1982-04-20

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