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JPS6152972B2 - - Google Patents
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JPS6152972B2 - - Google Patents

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Publication number
JPS6152972B2
JPS6152972B2 JP610878A JP610878A JPS6152972B2 JP S6152972 B2 JPS6152972 B2 JP S6152972B2 JP 610878 A JP610878 A JP 610878A JP 610878 A JP610878 A JP 610878A JP S6152972 B2 JPS6152972 B2 JP S6152972B2
Authority
JP
Japan
Prior art keywords
plane
single crystal
heat treatment
ions
silicon single
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
JP610878A
Other languages
Japanese (ja)
Other versions
JPS54100253A (en
Inventor
Kazumichi Oomura
Tomoyasu Inoe
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura Electric Co 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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP610878A priority Critical patent/JPS54100253A/en
Publication of JPS54100253A publication Critical patent/JPS54100253A/en
Publication of JPS6152972B2 publication Critical patent/JPS6152972B2/ja
Granted legal-status Critical Current

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

Description

【発明の詳細な説明】 この発明はイオン注入による不純物ドープ法を
用いた半導体装置の製造方法に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method of manufacturing a semiconductor device using an impurity doping method by ion implantation.

最近半導体への不純物ドープの方法、p―n接
合の製作の方法としてイオン注入法が広く用いら
れるようになつた。イオン注入法はドープ不純物
量の精度、均一性、誘電体被膜上からこの被膜の
下の半導体に不純物をドープ出来る等の特徴で従
来の拡散法に優つている。しかしイオン照射によ
る欠陥の発生等の欠点も有する。このために高温
でのアニール、或いは酸化雰囲気での高温での深
いドライブイン再拡散等が用いられて来た。最近
バイポーラ素子の高周波化、MOS素子の小形化
という観点から浅いp―n接合が望まれる。この
ような場合は重イオンである砒素(As)或いは
アンチモン(Sb)が用いられる。ところがAs,
Sbは重イオンのため、その飛程やその分散が小
さいが一方欠陥の発生も大きく900〜1100℃のア
ニールの際にこの多量の欠陥により増速拡散が起
り分布が拡がつてしまう効果があつた。
Recently, ion implantation has become widely used as a method for doping semiconductors with impurities and for manufacturing pn junctions. The ion implantation method is superior to the conventional diffusion method in terms of precision and uniformity of the amount of doped impurities, and the ability to dope the impurity from above the dielectric film to the semiconductor below this film. However, it also has drawbacks such as the occurrence of defects due to ion irradiation. For this purpose, high temperature annealing, high temperature deep drive-in re-diffusion in an oxidizing atmosphere, etc. have been used. Recently, shallow pn junctions have been desired from the viewpoint of increasing the frequency of bipolar devices and miniaturizing MOS devices. In such cases, heavy ions such as arsenic (As) or antimony (Sb) are used. However, As,
Since Sb is a heavy ion, its range and dispersion are small, but on the other hand, it also generates a large number of defects, and when annealing at 900 to 1100 degrees Celsius, this large amount of defects causes accelerated diffusion and has the effect of broadening the distribution. Ta.

他方半導体デバイス製作上からは浅いp―n接
合は次のような困難を生ずる。As或はSbをp型
シリコン(Si)単結晶表面近くにドープした浅い
n+型層の電極のために、アルミニウム(Al)を
蒸着、シンターすると、Al中にn+極層の部分の
Siがとけ込み、ピツト状の小穴が生じ、この小穴
中にAlが侵入し、Alがp型領域にまで突き抜け
てしまいp―n接合は整流性がなくなる。このよ
うなデバイス上の困難と半導体にイオン注入した
As,Sbの残留欠陥や深い再拡散を避けるため、
次のような方法が考案されている。この方法はSi
単結晶上に多結晶Siを推積させ、Asを多結晶内
のみ分布するような加速エネルギーでイオン注入
し、1000℃以上の高温で多結晶Si中から単結晶Si
中へ拡散させる方法である。Asをドープした多
結晶Siから単結晶SiにAsを拡散させる方法にお
いて、多結晶Si内の初期As濃度の均一性をイオ
ン注入で高めた方法で、Alの電極の問題も多結
晶Si厚を適当に厚くすることにより解決する。し
かし多結晶Si内から単結晶Siへの高温の拡散が依
然として必要である。
On the other hand, from the viewpoint of semiconductor device fabrication, shallow pn junctions cause the following difficulties. Shallow doping with As or Sb near the surface of p-type silicon (Si) single crystal
For the electrode of the n + type layer, when aluminum (Al) is evaporated and sintered, the part of the n + type layer is
The Si dissolves, creating pit-like holes, and Al enters into these holes, penetrating into the p-type region and causing the pn junction to lose its rectifying properties. Difficulties on such devices and ion implantation into semiconductors
To avoid residual defects and deep re-diffusion of As and Sb,
The following methods have been devised. This method uses Si
Polycrystalline Si is deposited on a single crystal, and As is ion-implanted with an acceleration energy that distributes only within the polycrystal.
This is a method of diffusing it inside. In the method of diffusing As from As-doped polycrystalline Si to single-crystalline Si, the uniformity of the initial As concentration in polycrystalline Si is increased by ion implantation, and the problem of Al electrodes can be solved by increasing the thickness of polycrystalline Si. This can be solved by making it appropriately thick. However, high-temperature diffusion from within polycrystalline Si to single-crystalline Si is still required.

この発明はこのような事情に鑑みてなされたも
ので、欠陥が少く浅い接合を形成でき且つイオン
注入層の電極を容易に取り得ることが可能な半導
体装置の製造方法を提供するものである。
The present invention has been made in view of the above circumstances, and it is an object of the present invention to provide a method for manufacturing a semiconductor device in which a shallow junction with few defects can be formed and an electrode of an ion-implanted layer can be easily obtained.

即ちこの発明は単結晶Si上に多結晶Siを堆積さ
せ、多結晶および単結晶双方に分布するように不
純物をイオン注入し、前記多結晶シリコスと対面
する前記シリコン単結晶の表面領域に全注入量の
5〜95%をドープせしめ、その後500〜650℃で第
一段階の熱処理を行なうことを特徴とする半導体
装置の製造方法である。
That is, in this invention, polycrystalline Si is deposited on single-crystal Si, impurity ions are implanted so as to be distributed in both the polycrystalline silicon and the single-crystal, and the entire surface region of the silicon single crystal facing the polycrystalline silicon is implanted. This method of manufacturing a semiconductor device is characterized in that it is doped by 5 to 95% of the amount of doping, and then a first stage heat treatment is performed at 500 to 650°C.

以下この発明の実施例を説明する。 Examples of the present invention will be described below.

先づ(100)面、もしくはこの面からの7゜以
内傾いたp型Si単結晶を用いこの単結晶を熱酸化
するか又はCVD法で〜5000ÅのSiO2膜を付着す
る。この後通常の光食刻法により窓をあけSi単結
晶面を露出する。次にSiH4の熱分解により多結
晶Si層を1000Å堆積する。この構造のウエハに
Asを200KVで3×1015ions/cm2イオン注入する。
この試料をN2中で500℃80分熱処理する。この熱
処理により単結晶中に生じたAsイオン注入によ
る欠陥が大部分回復する。すなわち非晶質層が単
結晶化しこれと同時にAsが電気的に回復する。
First, a p-type Si single crystal that is in the (100) plane or tilted within 7° from this plane is used, and a SiO 2 film of ~5000 Å is deposited on this single crystal by thermal oxidation or CVD. After this, a window is opened using a conventional photoetching method to expose the Si single crystal surface. Next, a polycrystalline Si layer of 1000 Å is deposited by thermal decomposition of SiH 4 . A wafer with this structure
As ions are implanted at 200 KV at 3×10 15 ions/cm 2 .
This sample is heat treated in N2 at 500°C for 80 minutes. This heat treatment recovers most of the defects caused by As ion implantation in the single crystal. That is, the amorphous layer turns into a single crystal, and at the same time, As recovers electrically.

この方法をn―p―nトランジスタのエミツタ
形成に使用した。即ちベース、コレクター接合が
表面から4000Åにあるような(100)エピタキシ
ヤルSiウエハのベース内に上記の方法でn+型のエ
ミツタ部を形成、上述の500℃80分熱処理後、
1000℃20分N2中で熱処理しAl電極を蒸着しシン
ターして形成し、n―p―nトランジスタを製作
した。1000℃20分の熱処理は多結晶Si層中のAs
の活性化と、単結晶Siの残留欠陥の回復に向けら
れている。このエミツタ・ベースの接合は2000Å
の位置に存在しその順方向電流電圧特性はI〜
exp(−qV/1.1×kT)と表わされた。又このト
ラン ジスタの2GHzでの雑音指数は2dBであつた。一方
同様のエピタキシヤルウエハに同様の多結晶Si層
を被着、同様のイオン注入を行ない、その後1000
℃20分、N2中で熱処理を行なつた場合はエミツ
タ・ベース接合が2500Åとなり、又ベース・コレ
クター接合は4800Åに後退したのが認められた。
そのI―V特性は、I〜qV/1.3×kTとなつた。
又2G Hzの雑音指数は2.5dBと増加した。又30kVで多結
晶Si層中に3×1015イオン/cm2のAsをイオン注入
し、その後1000℃、50分の熱処理によりAsをSi
単結晶に拡散させたものでは、コレクタ・ベース
接合が奥へ後退し、本発明のものに比べて高周波
遮断周波数が減少した。また(111)面或いは
(110)面のウエハを使用したときは、イオン注入
後550℃のアニールを2時間行ない、他は(100)
ウエハと全く同じプロセスで同様の結果が得られ
た。
This method was used to form the emitter of an npn transistor. That is, an n + type emitter part was formed in the base of a (100) epitaxial Si wafer with the base and collector junction located 4000 Å from the surface by the above method, and after the above heat treatment at 500°C for 80 minutes,
After heat treatment at 1000°C for 20 minutes in N 2 , an Al electrode was deposited and sintered to form an npn transistor. Heat treatment at 1000℃ for 20 minutes removes As in the polycrystalline Si layer.
It is aimed at the activation of single-crystal Si and the recovery of residual defects in single-crystal Si. This emitter-based junction is 2000Å
The forward current-voltage characteristics are I~
It was expressed as exp(−qV/1.1×kT). Also, the noise figure of this transistor at 2GHz was 2dB. On the other hand, a similar polycrystalline Si layer was deposited on a similar epitaxial wafer, and the same ion implantation was performed.
When heat treatment was performed at ℃ for 20 minutes in N 2 , the emitter-base junction was found to have a thickness of 2500 Å, and the base-collector junction was observed to have regressed to 4800 Å.
Its IV characteristic was I~qV/1.3×kT.
Also, the noise figure at 2G Hz increased to 2.5dB. In addition, 3×10 15 ions/cm 2 of As were ion-implanted into the polycrystalline Si layer at 30 kV, and then heat-treated at 1000°C for 50 minutes to transform the As into Si.
In the case of the one diffused into a single crystal, the collector-base junction retreated deep, and the high frequency cutoff frequency was reduced compared to the one of the present invention. Also, when using a (111) or (110) wafer, annealing at 550°C is performed for 2 hours after ion implantation, and for other (100) wafers.
Similar results were obtained using exactly the same process as for wafers.

上述した実施例では、多結晶シリコン層が1000
Åの場合に砒素イオンを200KVで加速し、単結晶
シリコン中にその一部がドープされるようにして
いる。しかしこれらに限ることなく、単結晶シリ
コン中へのドープ量が全くイオン注入量の5〜95
%であれば所定の効果が得られる。ここで単結晶
シリコン中への注入量が5%より少いと過剰なイ
オンが多結晶シリコンにドープされてしまう。従
つて接合形成のために高温熱処理が必要となり、
不純物プロフアイルの制御が困難になつて単結晶
シリコン内に浅い接合を作成できなくなつてしま
う。また、単結晶シリコン中への注入量が全注入
量の95%より多いと多結晶シリコン中にドープさ
れるイオンが極めて少くなつてしまい、多結晶シ
リコンが高抵抗なままになり、電極として使用で
きなくなる。
In the example described above, the polycrystalline silicon layer is 1000
In the case of Å, arsenic ions are accelerated at 200 KV so that a portion of them is doped into single crystal silicon. However, without being limited to these, the amount of doping into single crystal silicon may be 5 to 95% of the amount of ion implantation.
%, a predetermined effect can be obtained. If the amount of ions implanted into single crystal silicon is less than 5%, excessive ions will be doped into polycrystalline silicon. Therefore, high temperature heat treatment is required to form a bond.
The impurity profile becomes difficult to control, making it impossible to create shallow junctions in single-crystal silicon. In addition, if the amount of implantation into single crystal silicon is more than 95% of the total amount, the number of ions doped into polycrystalline silicon will be extremely small, and the polycrystalline silicon will remain highly resistive, making it difficult to use it as an electrode. become unable.

更に上述した実施列では、イオン注入後の熱処
理温度として500℃もしくは550℃を例示したが、
これに限らず熱処理温度は500〜650℃であれば所
定の効果が得られる。ここで熱処理温度が500℃
より低いと、シリコン単結晶中の欠陥の回復が不
十分となつてしまう。これにより、例えば後の高
温アニールの際に増速拡散を引き起こし接合が深
くなつてしまう。また、熱処理温度が650℃より
高くなると、単結晶シリコン中へ深く不純物が拡
散してしまい、やはり浅い接合の形成が困難にな
つてしまう。
Furthermore, in the above-mentioned embodiments, 500°C or 550°C was exemplified as the heat treatment temperature after ion implantation, but
The heat treatment temperature is not limited to this, but a predetermined effect can be obtained if the heat treatment temperature is 500 to 650°C. Here the heat treatment temperature is 500℃
If it is lower, the recovery of defects in the silicon single crystal will be insufficient. This causes accelerated diffusion during subsequent high-temperature annealing, resulting in a deeper bond. Furthermore, if the heat treatment temperature is higher than 650° C., impurities will diffuse deeply into the single crystal silicon, making it difficult to form shallow junctions.

上記の場合に於いて、特にイオンの注入量が5
×1015イオン/cm2以上と多くなると単結晶シリコ
ン中の欠陥の回復により高い熱処理が必要とな
る。即ち、単結晶シリコンの面方位が(100)
面、又は該面から7度以内の傾きを有する場合、
熱処理温度として550℃程度が必要で、又面方位
が(110)もしくは(111)面、又はそれらの面か
ら7度以内の傾きを有する場合、熱処理温度が
650℃程度が必要でこれより低温では単結晶シリ
ン中の欠陥の回復が不十分になることが確認され
た。
In the above case, especially when the ion implantation amount is 5.
When the amount exceeds ×10 15 ions/cm 2 , high heat treatment is required to recover defects in single crystal silicon. In other words, the plane orientation of single crystal silicon is (100)
plane, or has an inclination within 7 degrees from the plane,
Approximately 550℃ is required as the heat treatment temperature, and if the plane orientation is (110) or (111) plane or has an inclination within 7 degrees from these planes, the heat treatment temperature is
It was confirmed that a temperature of about 650°C is required, and that at lower temperatures, defects in single-crystal syringe are not fully recovered.

尚、上述した本発明において、(100)面、
(110)面、又は(111)面あるいはそれから7度
以内のシリコン単結晶面を用いる理由を述べる。
上記各面指数をもつ結晶面はそれら固有のすぐれ
た結晶学的、電気的性質をもつているが、結晶面
が上記各面から傾いて、±7度の傾きを越えると
他の面指数の結晶面の性質が顕著となつてしま
う。そこで本発明では上記(100)面、(110)面
又は(111)面もしくはこれら±7度以内の傾き
の結晶面を用いることにより、それら各面の本来
のすぐれた性質を生かしている。以上述べた本発
明の方法は、従来の方法に比べて優れた特性を有
するp―n接合或はn+―n接合を提供するもの
といえる。
In addition, in the present invention described above, the (100) plane,
The reason for using the (110) plane, the (111) plane, or a silicon single crystal plane within 7 degrees will be explained.
Crystal planes with the above plane indices have excellent crystallographic and electrical properties unique to them, but if the crystal plane is tilted from the above planes and exceeds an inclination of ±7 degrees, the crystal planes with the above plane indexes The properties of crystal planes become noticeable. Therefore, in the present invention, by using the above-mentioned (100) plane, (110) plane, or (111) plane, or a crystal plane having an inclination within ±7 degrees, the original excellent properties of each of these planes are utilized. It can be said that the method of the present invention described above provides a pn junction or an n + -n junction that has superior characteristics compared to conventional methods.

Claims (1)

【特許請求の範囲】 1 (100)面、(110)面、又は(111)面あるい
はそれらの面から7度以内の傾きを有するシリコ
ン単結晶面上に誘電体膜を形成し、この誘電体膜
を選択的に除去して前記シリコン単結晶を露出せ
しめ、少なくともこの露出したシリコン単結晶面
上に多結晶シリコン膜を形成し、この多結晶シリ
コン膜上からの砒素またはアンチモンのイオン注
入により、該多結晶シリコン膜と対面する前記シ
リコン単結晶の表面領域に全注入量の5〜95%を
ドープせしめ、その後500〜650℃で熱処理を行う
ことを特徴とする半導体装置の製造方法。 2 熱処理は2時間以内であることを特徴とする
特許請求の範囲第1項に記載の半導体装置の製造
方法。 3 イオン注入のドーズ量が5×1015イオン/cm2
以上で、シリコン単結晶が(110)面もしくは該
面から7度以内の傾きを有する場合、熱処理温度
を550℃程度に設定することを特徴とする特許請
求の範囲第1項に記載の半導体装置の製造方法。 4 イオン注入のドーズ量が5×1015イオン/cm2
以内で、シリコン単結晶が(110)又は(111)面
もしくはそれらの面から7度以内の傾きを有する
場合、熱処理温度を650℃程度に設定することを
特徴とする特許請求の範囲第1項に記載の半導体
装置の製造方法。
[Claims] 1. A dielectric film is formed on a (100) plane, a (110) plane, a (111) plane, or a silicon single crystal plane having an inclination of 7 degrees or less from these planes, and this dielectric film is Selectively removing the film to expose the silicon single crystal, forming a polycrystalline silicon film at least on the exposed silicon single crystal surface, and implanting arsenic or antimony ions from above the polycrystalline silicon film, A method for manufacturing a semiconductor device, characterized in that the surface region of the silicon single crystal facing the polycrystalline silicon film is doped with 5 to 95% of the total amount of doping, and then heat treatment is performed at 500 to 650°C. 2. The method for manufacturing a semiconductor device according to claim 1, wherein the heat treatment is performed for less than 2 hours. 3 Ion implantation dose is 5×10 15 ions/cm 2
In the above, when the silicon single crystal has a (110) plane or an inclination within 7 degrees from the plane, the semiconductor device according to claim 1, characterized in that the heat treatment temperature is set to about 550°C. manufacturing method. 4 Ion implantation dose is 5×10 15 ions/cm 2
Claim 1, characterized in that when the silicon single crystal has a (110) or (111) plane or an inclination within 7 degrees from these planes, the heat treatment temperature is set at about 650°C. A method for manufacturing a semiconductor device according to .
JP610878A 1978-01-25 1978-01-25 Manufacture of semiconductor device Granted JPS54100253A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP610878A JPS54100253A (en) 1978-01-25 1978-01-25 Manufacture of semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP610878A JPS54100253A (en) 1978-01-25 1978-01-25 Manufacture of semiconductor device

Publications (2)

Publication Number Publication Date
JPS54100253A JPS54100253A (en) 1979-08-07
JPS6152972B2 true JPS6152972B2 (en) 1986-11-15

Family

ID=11629294

Family Applications (1)

Application Number Title Priority Date Filing Date
JP610878A Granted JPS54100253A (en) 1978-01-25 1978-01-25 Manufacture of semiconductor device

Country Status (1)

Country Link
JP (1) JPS54100253A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58142303A (en) * 1982-02-17 1983-08-24 Sharp Corp Optical waveguide
JPS6484719A (en) * 1987-09-28 1989-03-30 Matsushita Electronics Corp Manufacture of semiconductor device

Also Published As

Publication number Publication date
JPS54100253A (en) 1979-08-07

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