JPS596505B2 - Method for diffusing impurities into semiconductor substrates - Google Patents
Method for diffusing impurities into semiconductor substratesInfo
- Publication number
- JPS596505B2 JPS596505B2 JP52016972A JP1697277A JPS596505B2 JP S596505 B2 JPS596505 B2 JP S596505B2 JP 52016972 A JP52016972 A JP 52016972A JP 1697277 A JP1697277 A JP 1697277A JP S596505 B2 JPS596505 B2 JP S596505B2
- Authority
- JP
- Japan
- Prior art keywords
- film
- silicon substrate
- semiconductor substrate
- diffusion
- impurities
- 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
Links
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- Formation Of Insulating Films (AREA)
- Bipolar Transistors (AREA)
Description
【発明の詳細な説明】
本発明は、三重拡散メサ型トランジスタのベース拡散処
理あるいは、整流素子のアノードもしくはカソード領域
を形成する拡散処理のように、半導体基板の一方の表面
全域から半導体基板内へ不純物を拡散する方法に関する
ものである。DETAILED DESCRIPTION OF THE INVENTION The present invention is directed to a diffusion process from one entire surface of a semiconductor substrate into the semiconductor substrate, such as a base diffusion process of a triple diffused mesa transistor or a diffusion process to form an anode or cathode region of a rectifying element. This invention relates to a method of diffusing impurities.
たとえば、三重拡散メサ型NPNトランジスタのベース
領域(第2図の4)の形成は、第1図で示すように、N
型シリコン基板1の一方の側にN+型の高不純物濃度領
域2を形成したのち、反対側の表面からP型の不純物を
全面拡散することによつて形成されるのが普通である。For example, the formation of the base region (4 in FIG. 2) of a triple diffused mesa type NPN transistor is as shown in FIG.
It is usually formed by forming an N+ type high impurity concentration region 2 on one side of the type silicon substrate 1, and then diffusing P type impurities over the entire surface from the opposite surface.
なお、このベース領域4を形成するためのP型不純物の
拡散に際しては、裏面に形成されたN+型拡散領域2か
らN型不純物が外部へ拡散するいわゆるアウトデイフユ
ージヨンを防止するとともに、P型の不純物がN+型領
域内へ拡散することを防止するべく、裏面全域を酸化膜
3で覆い、こののち拡散処理を施している。因に、N型
シリコン基板1は、表面が鏡面研磨され、一方、裏面が
JIS#1200ラップにより粗面化され、厚さが19
0μm程度の円板状であり、その裏面から燐を拡散して
形成したN+型拡散領域2は、拡散深さが約100tt
m、表面濃度が約1020C−lrL−3程度である。
ところで、かかるシリコン基板を、べ「ス拡散処理工程
で長時間にわたり高温(1200℃程度)加熱すると、
シリコン基板1とその裏面を覆う酸化膜3との熱膨張係
数が異るためにバイメタル現象が起り、ベース拡散処理
が施されたシリコン基板には反りが生じる。第2図は、
ベース領域が形成されたシリコン基板の体感を示す図で
、図示するようにP型ベース領域4の形成された側が凸
面となる如くシリコン基板は反る。かかるシリコン基板
の反りによつて、シリコン基板内には応力が発生し、拡
散処理工程でシリコン基板を収容する石英ボートとの接
触部分など応力の集中しやすい部分を起点にして、スリ
ップと称される格子欠陥が線状に発生する。第3図は、
その一般的な例であり、スリップライン5はシリコン基
板の周辺から結晶軸に沿つて直線的に発生する。Note that when diffusing P-type impurities to form this base region 4, it is necessary to prevent so-called out-diffusion, in which N-type impurities diffuse outside from the N+ type diffusion region 2 formed on the back surface, and to In order to prevent type impurities from diffusing into the N+ type region, the entire back surface is covered with an oxide film 3, and then a diffusion process is performed. Incidentally, the front surface of the N-type silicon substrate 1 is mirror polished, while the back surface is roughened by JIS #1200 lapping and has a thickness of 19 mm.
The N+ type diffusion region 2, which has a disc shape of approximately 0 μm and is formed by diffusing phosphorus from the back surface, has a diffusion depth of approximately 100 tt.
m, and the surface concentration is about 1020C-lrL-3.
By the way, if such a silicon substrate is heated at a high temperature (about 1200°C) for a long time in the base diffusion treatment process,
Since the thermal expansion coefficients of the silicon substrate 1 and the oxide film 3 covering the back surface thereof are different, a bimetal phenomenon occurs, and the silicon substrate subjected to the base diffusion process is warped. Figure 2 shows
This is a diagram illustrating the physical sensation of a silicon substrate on which a base region is formed. As shown in the figure, the silicon substrate is warped so that the side on which the P-type base region 4 is formed becomes a convex surface. This warping of the silicon substrate generates stress within the silicon substrate, which is called slip, which occurs in areas where stress tends to concentrate, such as the contact area with the quartz boat that houses the silicon substrate during the diffusion process. Linear lattice defects occur. Figure 3 shows
As a general example, the slip line 5 is generated linearly from the periphery of the silicon substrate along the crystal axis.
また、シリコン基板の裏面を覆う酸化膜の厚みを増すこ
とによつて、強いバイメタル現象を起すと、応力は、基
板の中心部に集中し、第4図で示すようにスリツプライ
ン5は中心部にあられれ、周辺部では減少する傾向を示
す。このスリツプラインは、結晶格子が結晶軸面に沿つ
て辷り、この辷つた面に沿つて結晶格子がくずれて生じ
るものであり、エツチングによつて、エツチピツトが連
つて発生することから容易に観察できる。このようなス
リツプラインを持つシリコン基板でトランジスタを製作
した場合、欠陥面が電流担体の再結合中心の群として作
用するため、製作されたトランジスタの耐電圧特性の劣
化、リーク電流の増加あるいは電流増幅率の低下など幾
多の不都合が生じる。Furthermore, if a strong bimetal phenomenon is caused by increasing the thickness of the oxide film covering the back surface of the silicon substrate, stress will be concentrated at the center of the substrate, and the slip line 5 will be at the center as shown in FIG. It shows a tendency to decrease in the peripheral areas. This slip line is caused by the crystal lattice stretching along the crystal axis plane, and the crystal lattice collapses along the stretched plane, and can be easily observed because etching pits are generated in succession due to etching. . When a transistor is manufactured using a silicon substrate with such slip lines, the defective surface acts as a group of recombination centers for current carriers, resulting in deterioration of the withstand voltage characteristics of the manufactured transistor, increase in leakage current, or current amplification. Many inconveniences occur, such as a decrease in the rate.
本発明は、上記の不都合を排除するべくなされたもので
あり、半導体基板の片側にのみ全面拡散処理を施す拡散
処理工程で顕著になるバイメタル現象を抑圧することが
でき、したがつて、半導体基板の反りに起因するスリツ
プラインの発生を阻止することのできる半導体基板への
不純物の拡散方法を提供するものである。The present invention has been made in order to eliminate the above-mentioned disadvantages, and can suppress the bimetal phenomenon that becomes noticeable in the diffusion treatment process in which the entire surface diffusion treatment is performed only on one side of the semiconductor substrate. The purpose of the present invention is to provide a method for diffusing impurities into a semiconductor substrate, which can prevent the occurrence of slip lines due to warping of the semiconductor substrate.
本発明の特徴は、一方の面が酸化膜で覆われてなる半導
体基板の他方の面よりN型もしくはP型不純物を全面拡
散するにあたり、半導体基板の一方の面を覆う酸化膜よ
り薄い酸化膜または窒化膜等の被膜で半導体基板の他方
の面全域を覆い、同被膜を通しての不純物の拡散をなす
ことにある。A feature of the present invention is that when an N-type or P-type impurity is diffused over the entire surface of a semiconductor substrate whose one surface is covered with an oxide film, an oxide film that is thinner than the oxide film that covers one surface of the semiconductor substrate is used. Alternatively, the entire other surface of the semiconductor substrate may be covered with a film such as a nitride film, and impurities may be diffused through the film.
以下に図面を参照して本発明を詳細に説明する。第5図
は、本発明の方法によりベース拡散領域が形成される三
重拡散メサ型NPNトランジスタのベース拡散処理を施
す直前の状態を示す図であり、図示するように、N型シ
リコン基板1の表面全域には、裏面すなわちN+型拡散
領域2の表面全域を覆う酸化膜3よりも薄い被覆たとえ
ば絶縁被膜6が形成されている。第6図は、第5図で示
したシリコン基板に対してP型不純物たとえば硼素を用
いたベース拡散処理を施した後のシリコン基板の断面図
であり、図示するように、薄い絶縁被膜6を通して硼素
がN型シリコン基板1の中へ拡散し、P型ベース領域7
が形成される〇かかる本発明の方法によれば、シリコン
基板と酸化膜3との熱膨張係数の差に基くバイメタル現
象は依然として発生してはいるが、シリコン基板1と絶
縁被膜6との熱膨張係数の差に基くバイメタル現象が新
たに発生しており、しかも両現象によつて半導体基板に
これを反らせるべく作用する力の方向が相反する方向で
あるため、これらが相殺し合い、したがつて、シリコン
基板1には、スリツプラインが発生するほどの反りは発
生しない。The present invention will be described in detail below with reference to the drawings. FIG. 5 is a view showing the state immediately before base diffusion treatment of a triple diffusion mesa type NPN transistor in which a base diffusion region is formed by the method of the present invention. A coating, for example, an insulating coating 6, which is thinner than the oxide film 3 covering the back surface, that is, the entire surface of the N+ type diffusion region 2, is formed over the entire area. FIG. 6 is a cross-sectional view of the silicon substrate shown in FIG. 5 after a base diffusion process using a P-type impurity such as boron is performed, and as shown, a thin insulating film 6 is passed through the silicon substrate. Boron diffuses into the N-type silicon substrate 1 and forms the P-type base region 7.
According to the method of the present invention, although the bimetal phenomenon based on the difference in thermal expansion coefficient between the silicon substrate 1 and the oxide film 3 still occurs, the heat between the silicon substrate 1 and the insulating film 6 is A new bimetal phenomenon based on the difference in expansion coefficient has occurred, and since the directions of the forces acting on the semiconductor substrate to warp it due to both phenomena are opposite, they cancel each other out, and therefore , the silicon substrate 1 does not warp to the extent that a slip line occurs.
ところで、本発明の方法では、被膜を通して不純物の拡
散がなされるため、技術的に考慮しなければならない事
柄が発生する。すなわち、絶縁被膜6を形成するにあた
り、膜厚をこの膜とシリコン基板との間で生じるバイメ
タル現象の強さが、酸化膜3とシリコン基板との間で生
じ。るバイメタル現象の強さと同等程度となり、しかも
、絶縁被膜を通して不純物の拡散が可能である厚さに選
定することである。次表は、次のような条件をみたす膜
厚を検討するため、裏面に1,2μmの酸化膜が形成さ
れてなるシリコン基板の表面に形成する絶縁被膜(Si
O2膜)の厚みを変化させ、封管法を駆使して1200
℃の温度下で8時間にわたり硼素の拡散を行つた実験結
果を示す。By the way, in the method of the present invention, since impurities are diffused through the film, there are some technical issues that must be taken into account. That is, when forming the insulating film 6, the strength of the bimetal phenomenon that occurs between the film and the silicon substrate occurs between the oxide film 3 and the silicon substrate. The thickness should be selected to be equivalent to the strength of the bimetal phenomenon caused by the insulating film, and to allow diffusion of impurities through the insulating film. The following table shows the insulating film (Si
1200 by changing the thickness of the O2 film) and making full use of the sealing tube method.
The results of an experiment in which boron was diffused for 8 hours at a temperature of .degree. C. are shown.
なお、管内に配置した不純物源の硼素濃度は、2.5×
1020cTn−3に調整され、また、炉温は、徐熱徐
冷するプログラムで制御され、急激な温度変化による影
響を避けた。The boron concentration of the impurity source placed inside the tube is 2.5×
The furnace temperature was adjusted to 1020 cTn-3, and the furnace temperature was controlled by a slow heating and slow cooling program to avoid the effects of sudden temperature changes.
この結果から明らかなように、膜厚が300λ以上にな
るとスリツプラインの発生を抑圧する効果がみられる。As is clear from this result, when the film thickness is 300λ or more, there is an effect of suppressing the occurrence of slip lines.
また、膜厚の上限は、基本的には、裏面の酸化膜の厚み
より小であればよいが、あまり厚くした場合には、拡散
領域の表面不純物濃度が低くなり、拡散領域へ直接電極
を付設した場合の接触抵抗が高くなる。良好な接触状態
を得るために必要な表面不純物濃度は1018?−3程
度以上であり、このこととスリツプライン発生の抑圧効
果を考慮した場合、絶縁被膜6の厚みを1000八〜3
000人程度に選定することが効果的である。以上説明
してきたように、本発明の方法によれば、スリツプライ
ンの発生を抑圧して全面拡散処理を半導体基板に施すこ
とが可能になる。In addition, the upper limit of the film thickness should basically be smaller than the thickness of the oxide film on the back side, but if it is made too thick, the surface impurity concentration of the diffusion region will decrease, and the electrode cannot be directly connected to the diffusion region. Contact resistance increases when attached. Is the surface impurity concentration required to obtain good contact conditions 1018? -3 or more, and considering this and the effect of suppressing the generation of slip lines, the thickness of the insulating coating 6 should be approximately 1000 to 3.
It is effective to select approximately 000 people. As described above, according to the method of the present invention, it is possible to suppress the occurrence of slip lines and to perform a full-surface diffusion process on a semiconductor substrate.
なお、本発明はその目的からして、バイメタル現象が生
じ不純物の拡散が可能な被膜であれば酸化膜、窒化膜等
の絶縁膜以外の被膜を使用することも当然可能である。
以上の説明は、不純物として硼素を用いた場合を例にな
されたのであるが、他の不純物、例えば、燐、砒素、ア
ルミニウムを用いることもできる。特に、不純物として
アルミニウムを用いた場合には、絶縁被膜の厚さが20
00八程度までは、不純物源の濃度を高めなくても、絶
縁被膜のない場合と同程度の表面不純物濃度の得られる
ことが確認された。さらに、本発明は、開管法にも適用
可能であり、開管法による場合は、半導体基板の配置さ
れた雰囲気中には不純物が過剰に存在するため、封管法
による場合のように不純物源の量に留意する必要はない
。Note that, in view of the purpose of the present invention, it is of course possible to use a film other than an insulating film such as an oxide film or a nitride film as long as it is a film that causes a bimetal phenomenon and allows diffusion of impurities.
Although the above description has been made using boron as an example of the impurity, other impurities such as phosphorus, arsenic, and aluminum can also be used. In particular, when aluminum is used as an impurity, the thickness of the insulating film is 20
It was confirmed that up to about 0.08, a surface impurity concentration comparable to that without an insulating film could be obtained without increasing the concentration of the impurity source. Furthermore, the present invention can also be applied to an open tube method; in the case of the open tube method, impurities are excessively present in the atmosphere in which the semiconductor substrate is placed; There is no need to pay attention to the amount of source.
また、半導体基板はシリコンに限られるものではなく、
ゲルマニウム基板あるいは化合物半導体基板であつても
よい。Furthermore, semiconductor substrates are not limited to silicon;
It may be a germanium substrate or a compound semiconductor substrate.
さらに、本発明の拡散方法は、上記の実施例で示した三
重拡散メサ型トランジスタのベース拡散工程のみならず
、全面拡散処理によつて所定の領域を形成する工程、た
とえば、整流素子のアノードまたはカソード拡散処理工
程、などにも適用しうること勿論である。Furthermore, the diffusion method of the present invention is applicable not only to the step of base diffusion of the triple diffused mesa transistor shown in the above embodiment, but also to the step of forming a predetermined region by full-surface diffusion treatment, such as the step of forming a predetermined region on the anode of a rectifying element or Of course, it can also be applied to cathode diffusion treatment steps, etc.
第1図および第2図は従来の方法による三重拡散メサ型
NPNトランジスタのベース領域の形成工程とベース領
域形成後の状態について説明するための図、第3図およ
び第4図は従来の方法により拡散処理のなされたシリコ
ン基板におけるスリツプラインの発生状態を示す略図、
第5図および第6図は本発明の方法による三重拡散メサ
型NPNトランジスタのベース領域の形成工程とベース
領域形成後の状態について説明するための図である。
1・・・・・・N型シリコン基板、2・・・・・・N+
型拡散領域、3・・・・・・酸化膜、6・・・・・・絶
縁被膜、7・・・・・・P型ベース領域。1 and 2 are diagrams for explaining the process of forming the base region of a triple diffused mesa type NPN transistor by the conventional method and the state after the base region is formed. A schematic diagram showing the state of occurrence of slip lines in a silicon substrate subjected to diffusion treatment,
FIGS. 5 and 6 are diagrams for explaining the step of forming a base region of a triple diffused mesa type NPN transistor according to the method of the present invention and the state after the base region is formed. 1...N-type silicon substrate, 2...N+
Type diffusion region, 3... Oxide film, 6... Insulating film, 7... P type base region.
Claims (1)
覆われた半導体基板の他方の面から、ドナーもしくはア
クセプタ不純物を全面拡散するにあたり、前記酸化膜の
厚さより薄く、かつ、膜厚が300Å〜2000Åの範
囲に選定された被膜を前記半導体基板の他方の面全域に
形成し、こののち、同被膜を通して不純物を全面拡散し
、前記半導体基板の他方の表面層全域に電極接触が可能
な表面不純物濃度をもつ拡散領域を形成することを特徴
とする半導体基板への不純物の拡散方法。1. When diffusing donor or acceptor impurities over the entire surface from the other surface of a semiconductor substrate, one surface of which is covered with an oxide film having a thickness that prevents impurity from passing through, A film with a thickness selected to be in the range of 300 Å to 2000 Å is formed over the entire other surface of the semiconductor substrate, and then impurities are diffused over the entire surface through the film, so that electrode contact can be made over the entire other surface layer of the semiconductor substrate. A method for diffusing impurities into a semiconductor substrate, the method comprising forming a diffusion region having a surface impurity concentration.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP52016972A JPS596505B2 (en) | 1977-02-17 | 1977-02-17 | Method for diffusing impurities into semiconductor substrates |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP52016972A JPS596505B2 (en) | 1977-02-17 | 1977-02-17 | Method for diffusing impurities into semiconductor substrates |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS53101977A JPS53101977A (en) | 1978-09-05 |
| JPS596505B2 true JPS596505B2 (en) | 1984-02-13 |
Family
ID=11930980
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP52016972A Expired JPS596505B2 (en) | 1977-02-17 | 1977-02-17 | Method for diffusing impurities into semiconductor substrates |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS596505B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS626009U (en) * | 1985-06-27 | 1987-01-14 |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63144517A (en) * | 1986-12-09 | 1988-06-16 | Nec Corp | Manufacture of semiconductor device |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5922373B2 (en) * | 1973-09-07 | 1984-05-26 | 株式会社日立製作所 | Semiconductor wafer processing method |
-
1977
- 1977-02-17 JP JP52016972A patent/JPS596505B2/en not_active Expired
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS626009U (en) * | 1985-06-27 | 1987-01-14 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS53101977A (en) | 1978-09-05 |
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