JPS6119104B2 - - Google Patents
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- JPS6119104B2 JPS6119104B2 JP54154309A JP15430979A JPS6119104B2 JP S6119104 B2 JPS6119104 B2 JP S6119104B2 JP 54154309 A JP54154309 A JP 54154309A JP 15430979 A JP15430979 A JP 15430979A JP S6119104 B2 JPS6119104 B2 JP S6119104B2
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Classifications
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10P—GENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
- H10P95/00—Generic processes or apparatus for manufacture or treatments not covered by the other groups of this subclass
- H10P95/90—Thermal treatments, e.g. annealing or sintering
Landscapes
- Bipolar Transistors (AREA)
- Thyristors (AREA)
Description
本発明はトランジスタ、サイリスタ等の個別素
子或いはバイポーラ集積回路(以下バイポーラ
ICと称する)等の半導体素子の製造方法に関す
る。
一般にトランジスタ、サイリスタ或いはバイポ
ーラIC等の半導体素子は主として高速性、高利
得及び低熱損失が要求される。特に個別素子に
は、応用装置の小型化、大容量化の為に上記性能
の他に高電流、高耐圧が要求される。これらの性
能は素子の内部の構成で決まることが多く、それ
らの性能の間には各々トレードオフの関係があ
る。例えば高速性を改良するには中性領域のライ
フタイムを低くし、各半導体層の厚さを小さくす
る必要があるが、ライフタイムを低くすると電流
利得が下がり、オン電圧が増加して熱損失の増加
を招き、また半導体層の厚さを小さくすると高耐
圧が得られないというように性能の間に各々トレ
ードオフの関係がある。そして実際、半導体素子
は用途に応じて各特性間のトレードオフ点の最適
化を行なつている。
しかし素子のパラメータの中にはトレードオフ
関係外のものもあり、例えば制御電極を有する半
導体層内の少数キヤリアライフタイムは、高けれ
ば高い程この層をベースとするトランジスタの電
流増幅率が増加し、スイツチング性能が向上する
と共にオン電圧が低くなり、さらにリーク電流も
減少するというように素子性能がほとんど改善さ
れる。従つて個別素子或いはバイポーラIC等の
半導体素子においては一般に半導体基体のキヤリ
アライフタイムをでき限り高くすることが望まし
い。
しかしながら実際の製造プロセスでは半導体基
体に不純物を導入するために、拡散等の1000℃以
上の高温熱処理が行われることによつて、熱処理
中に容器から混入する重金属や熱処理瞳によつて
半導体基体に生ずる熱ひずみのにより、キヤリア
のトラツプ準位が作られ、キヤリアライフタイム
を低くしている。この現象は、ライフタイムキラ
ー原子の拡散のような意識的なライフタイム制御
と異なり、素子性能の劣化や素子製造の再現性の
低下を引き起す主因となつてきた。
この問題の解決法の一つとしてリンゲツター法
が良く知られている。これはリン化合物を半導体
基体上に形成(デポジシヨン)し、リン化合物の
リンを半導体基体中に拡散する時に、半導体基体
中に含まれるFe,Cuなどの重金属が熱によつて
拡散し、半導体基体上のリン化合物層に吸着さ
れ、その結果半導体基体中の重金属が減少し、ラ
イフタイムが高くなるという効果を利用したもの
である。このリンゲツター効果を利用した方法
を、第1図a〜dを参照して具体的に説明する。
この第1図a〜dに示すのは個別素子の一つサイ
リスタの製造工程の一例である。まずn型Si基板
11の両側より例えばGaを拡散してアノード層
となるp型層12と後にゲート電極が形成されp
ベース層となるp型層13とを形成してp−n−
p構造のSi基体11を得る(第1図a)。次にp
ベース層となるp型層13上にリンガラス層14
を形成(デポジシヨン)する(第1図b)。この
リンガラス層14形成時に、Si基体中に含む重金
属及び外部にある重金属がリンガラス層14に吸
着する。この後リンガラス層14を除去し、Si基
体11表面近傍に含むリンを拡散してカソード層
となるn型層15を形成する(第1図c)。なお
この工程でリンガラス層14を除去した後にリン
を拡散するのはカソード層となるn型層の表面濃
度、深さを制御する為である。しかる後アノード
層となるp型層12側よりライフタイムキラー原
子(図中点々で示す)を拡散する(第1図d)。
最後に図示してないが、アノード層となるp層1
2にアノード電極、pベース層となるp型層13
にゲート電極、カソード層となるn型層15にカ
ソード電極を形成してサイリスタ素子が得られ
る。
このようにして得られたサイリスタ素子は、リ
ンゲツター効果を利用している為、、Si基体11
中の重金属の量が減少しライフタイムが向上す
る。しかしながらライフタイムが向上するのは、
わずかであつて、結果的にリンゲツター効果を利
用しない方法のサイリスタとほとんど変りがな
い。この理由として考えられることは、リンを拡
散する時にリンガラス層14が形成されていない
為、Si基体11表面付近に吸引された重金属が、
リンを拡散する時に再拡散され、Si基体11中に
侵入する為である。このようにリンガラス層の形
成(デポジシヨン)時に一度ライフタイムを上げ
て置きながら、リンの拡散時にキヤリアライフタ
イムを下げるという製造工程における致命的な欠
点があつた。
本発明は上記した欠点に鑑みなされたもので、
キヤリアライフタイムを高くし諸特性を良くした
半導体素子の製造方法を提供するものである。
即ち本発明は半導体基体中にリン(n型不純
物)を拡散した後、該半導体基体の少なくとも一
方の面にリンを透過し、且つ半導体基体にリンが
拡散されない厚さの薄膜を形成し、しかる後半導
体基体をリンを含む雰囲気中で熱処理して再びラ
イフタイムを向上せしめる方法である。
以下図面を参照して本発明の一実施例を説明す
る。第2図a〜eは本発明の一実施例であつて、
第1図に対応してサイリスタの製造工程を示す工
程断面図である。こ第2図のa〜c迄は第1図の
a〜cと同様である。即ちまずn型Si基板11の
両側よりGaを拡散してアノード層となるp型層
12と後にゲート電極が形成されpベース層とな
るるp型層13とを形成してp−n−p構造のSi
基体11を得る(第2図a)。次にpベース層と
なるp型層13上にリンガラス層14を形成(デ
ポジシヨン)する(第2図b)。この時通常アノ
ード層となるp型層12側を図示してないが
SiO2膜等で被覆して置く。このリンガラス層1
4形成時に、Si基体中に含む重金属及び外部にあ
る重金属がリンガラス層14に吸着する。従つて
この工程でSi基体特にpベース層となるp型層の
ライフタイムは、後に説明する如く数十倍向上す
る。この後リンガラス層14を除去し、Si基体1
1に含むリンを1200℃位の温度で5時間位拡散し
てカソード層となるn型層15を形成する(第2
図c)。このリンを拡散する工程で、従来例で述
べた如くSi基体表面近傍に吸引されていた重金属
がSi基体中に再拡散され、Si基体特にpベース層
となるp型層13のライフタムが下がり、後に説
明(第5図)する如く元の値にもどつてしまう。
ここ迄が従来即ち第1図と同様な方法である。次
の工程が本発明の重要な工程である。即ちリンを
をSi基体所謂るpベース層となるp型層13に拡
散した後、リンを透過しなおかつ基体にリンが拡
散されない厚さの熱酸化膜26をアノード層とな
るp型層12に形成し、これをリンを含む雰囲気
中で熱処理する工程である(第2図d)。例えば
熱酸化膜26を5000Å形成しリンを含む雰囲気中
1000℃で1時間の熱処理を行う。ここで熱酸化膜
はアノード層となるp型層12にのみ形成すると
したが、カソード層となるn型層15に形成して
も勿論問題はなく。たとえば、プレーナー型素子
などの如く表面にp型層が露出しているような半
導体素子においては当然リンが半導体基体に拡散
するのを防ぐためにも両面に熱酸化膜を形成すべ
きである。このようにリンを含む雰囲気中でシリ
コン基体11を処理すると、、リンの拡散工程で
下がつたライフタイムが再び向上し、後に説明
(第5図)する如くリンの拡散直後の数十倍向上
する。しかる後熱酸化膜26を除去し第1図dの
工程と同様にアノード層となるp型層12側より
ライフタイムキラー原子であるAu原子(図中
点々で示す)を拡散する。最後に図示してないが
従来例と同様アノード層となるp型層12にアノ
ード電極、pベース層となるp型層13にゲート
電極、カソード層となるn型層15にカソート電
極を形成しててサイリスタ素子が得られる。
第3図a〜eは本発明の他のの実施例であつ
て、第1図に対応してサイリスタの製造工程を示
す工程断面図である。この第3図のa〜c迄は第
1図のa〜cと同様である。即ちまずn型Si基板
11の両側よりGaを拡散してアノード層となる
p型層12と後にゲート電極が形成されpベース
層となるp型層13とを形成してp−n−p構造
のSi基体11を得る(第3図a)。次にpベース
層となるp型層13上にリンガラス層14を形成
(デポジシヨン)する(第3図b)。この時通常ア
ノード層となるp型層12側を図示してないが
SiO2膜等で被覆して置く。このリンガラス層1
4形成時に、Si基体中に含む重金属及び外部にあ
る重金属がリンガラス層14に吸着する。従つて
この工程でSi基体特にpベース層となるp型層の
ライフタイムは、後に説明する如く数十倍向上す
る。この後リンガラス層14を除去し、Si基体1
1に含むリンを1200℃位の温度で5時間位拡散し
てカソード層となるn型層15を形成する(第3
図c)。このリンを拡散する工程で、従来例で述
べた如くSi基体表面近傍に吸引されていた重金属
がSi基体中に再拡散され、Si基体特にpベース層
となるp型層13のライフタイムが下がり、後に
説明(第5図)する如く元の値にもどつてしま
う。ここ迄が従来即ち第1図と同様な方法であ
る。次の工程が本発明の重要な工程である。即ち
リンをSi基体所謂るpベース層となるp型層13
に拡散した後、リンを透過しなおかつ基体にリン
が拡散されない厚さの低温酸化膜37をアノード
層となるp型層12に形成し、これをリンを含む
雰囲気中で熱処理する工程である(第3図d)。
例えばCVD法などを用いて低温酸化膜37を
5000Å形成し、リンを含む雰囲気中1000℃で1時
間の熱処理を行う。ここで低温酸化膜はアノード
層となるp型層12にのみ形成するとしたが、カ
ソード層となるn型層15に形成しても勿論問題
はなく、たとえば、プレーナー型素子などの如く
表面にp型層が露出しているような半導体素子に
おいては当然リンが半導体基体に拡散するのを防
ぐためにも両面に低温酸化膜を形成すべきであ
る。このようにリンを含む雰囲気中でシリコン基
体11を処理すると、リンの拡散工程で下がつた
ライフタイムが再び向上し、後に説明(第5図)
する如くリンの拡散直後の数十倍向上する。しか
る後低温酸化膜37を除去し第1図dの工程と同
様にアノード層となるp型層12側よりライフタ
イムキラー原子であるAu原子(図中点々で示
す)を拡散する。最後に図示してないが従来例と
同様アノード層となるp型層12にアノード電
極、pベース層となるp型層13にゲート電極、
カソード層となるn型層15にカゾード電極を形
成してサイリスタ素子が得られる。
第4図a〜eは本発明の他の実施例であつて、
第1図に対応してサイリスタの製造工程を示す工
程断面図である。この第4図のa〜c迄は第1図
のa〜cと同様である。即ちまずn型Si基体11
の両側よりGaを拡散してアノード層となるp型
層12と後にゲート電極が形成されpベース層と
なるp型層13とを形成してp−n−p構造のSi
基体11を得る(第4図a)。次にpベース層と
なるp型層13上にリンガラス層14を形成(デ
ポジシヨン)する(第4図b)この時通常アノー
ド層となるp型層12側を図示してないがSiO2
膜等で被覆して置く。このリンガラス層14形成
時に、Si基体中に含む重金属及び外部にある重金
属がリンガラス層14に吸着する。従つてこの工
程でSi基体特にpベース層となるp型層のライフ
タイムは、後に説明する如く数十倍向上する。こ
の後リンガラス層14除去し、Si基体11に含む
リンを1200℃位の温度で5時間位拡散してカソー
ド層となるn型層15を形成する(第4図c)。
このリンを拡散する工程で、従来例で述べた如く
Si基体表面近傍に吸引されていた重金属がSi基体
中に再拡散され、Si基体特にpベース層となるp
型層13のライフタイイムや下がり、後に説明
(第3図)する如く元の値にもどつてしまう。こ
こ迄が従来即ち第1図と同様な方法である。次に
工程が本発明の重要な工程である。即ちリンをSi
基体所謂るpベース層となるp型層13に拡散し
た後、リンを透過しなおかつ基体にリンが拡散さ
れない厚さの多結晶シリコン膜48をアノード層
となるp型層12に形成し、これをリンを含む雰
囲気中で熱処理する工程である(第2図d)。こ
こで多結晶シリコン膜はアノード層となるp型層
12にのみ形成するとしたが、カソード層となる
n型層15に形成しても勿論問題はなく、たとえ
ば、プレーナー型素子などの如く表面にp型層が
露出しているような半導体素子においては当然リ
ンが半導体基体に拡散するのを防ぐためにも両面
に多結晶シリコン膜を形成すべきである。このよ
うにリンを含む雰囲気中でシリコン基体11を処
理すると、リンの拡散工程で下がつたライフタイ
ムが再び向上し、後に説明(第3図)する如くリ
ンの拡散直後の数十倍向上する。しかる後多結晶
シリコン膜48を除去し第1図dのの工程と同様
にアノード層となるp型層12側よりライフタイ
ムキラー原子であるAu原子(図中点々で示す)
を拡散する。最後に図示していないが従来例と同
様アノード層となるp型層12にアノード電極、
pベース層となるp型層13にゲート電極、カソ
ード層となるn型層15にカソード電極を形成し
てサイリスタ素子が得られる。
このようにして得られたサイリスタ素子は、従
来即ち第1図a〜dのようにして得られたサイリ
スタ素子に比べ、Si基体特にpベース層となるp
型層のライフタイムが高く良好なスイツチング特
性を有するようになる。
次に、上記実施例の如く得られたサイリスタ素
子のSi基体即ちpベース層となるp型層13のラ
イフタイムが、従来即ち第1図a〜dのようにし
て得られたサイリスタ素子のpベース層となるp
型層13のライフタイムより、具体的にどの程度
良好であるかを第2図の実施例を用いて第5図を
参照して説明する。この第5図は従来の第1図a
〜d及び本発明一実施例の第2図a〜eに対応の
a′〜d′,a″〜e″に対するサイリスタ素子のnベー
ス層となるn型層11のライフタイム(μsec)
を示した曲線図で、点線が従来の場合、実線が本
発明一実施例の場合である。この第5図から明ら
かなように、従来の場合はSi基体のnベース層と
なるn型層のライフタムが0.6〜1.1μsec・位
で、一方本発明の一実施例の場合はn型層のライ
フタイムが1.1〜1.3μsec・位であつた。即ち従
来の場合は目標値の1.2μsec.にみたないものが
多く且つバラツキが大きかつた。これに対し本発
明の一実施例の場合は目標値の値にほとんど達成
し且つバラツキも少なかつた。このようにライフ
タイムが目標値にほとんど達成し且つバラツキも
少なく(再現性が良い)なつた理由としては、上
述した如くリンを拡散した後に再びリンを透過す
る薄膜でマスクしたシリコン半導体基体11をリ
ンを含む雰囲気中で熱処理することによつて、Si
基体中に再拡散された重金属及び外部の重金属が
再び雰囲気中のリンによつて吸着され、この後に
850℃位の温度で金拡散を施しても、リンを拡散
する直後のSi基体中の重金属が少なくらる為であ
る。なお第5図におけるライフタイムの測定は闘
ダイオード電圧降下法によつて行つたもので、又
この第5図に示すのは700℃上の熱処理工程を有
する所のライフタイムの変化である。このように
nベース層となるn型層のライフタイムはほぼ目
標値になるが、pベース層となるp型層13ライ
フタイムは残念ながら直接測定する手段が現在の
ところ見当らないが、n型層のライフタイムから
計算により求める方法や素子特性から類推する方
法により十分に判る。よく用いられる計算式は
The present invention applies to individual elements such as transistors and thyristors, or bipolar integrated circuits (hereinafter referred to as bipolar integrated circuits).
This invention relates to a method for manufacturing semiconductor devices such as ICs. Generally, semiconductor devices such as transistors, thyristors, and bipolar ICs are required to have high speed, high gain, and low heat loss. In particular, individual elements are required to have high current and high voltage resistance in addition to the above-mentioned performance in order to miniaturize and increase capacity of applied devices. These performances are often determined by the internal configuration of the element, and there is a trade-off relationship between these performances. For example, to improve high speed, it is necessary to lower the lifetime of the neutral region and reduce the thickness of each semiconductor layer, but lowering the lifetime reduces current gain, increases on-state voltage, and causes heat loss. There is a trade-off relationship between the performances, such as an increase in the semiconductor layer thickness, and a reduction in the thickness of the semiconductor layer makes it impossible to obtain a high breakdown voltage. In fact, the trade-off point between each characteristic of a semiconductor device is optimized depending on the application. However, some device parameters are outside the trade-off relationship; for example, the higher the minority carrier lifetime in the semiconductor layer containing the control electrode, the higher the current amplification factor of the transistor based on this layer. , the switching performance is improved, the on-voltage is lowered, and the leakage current is also reduced, so that the device performance is almost improved. Therefore, in semiconductor devices such as individual devices or bipolar ICs, it is generally desirable to make the carrier lifetime of the semiconductor substrate as high as possible. However, in the actual manufacturing process, high-temperature heat treatment of over 1000℃ such as diffusion is performed to introduce impurities into the semiconductor substrate. The resulting thermal strain creates a carrier trap level, reducing the carrier lifetime. This phenomenon, unlike intentional lifetime control such as the diffusion of lifetime killer atoms, has been a major cause of deterioration of device performance and reproducibility of device manufacturing. The Ringetter method is well known as one of the solutions to this problem. This is because a phosphorus compound is formed (deposited) on a semiconductor substrate, and when the phosphorus in the phosphorus compound is diffused into the semiconductor substrate, heavy metals such as Fe and Cu contained in the semiconductor substrate are diffused by heat, and the semiconductor substrate is heated. This takes advantage of the effect that heavy metals are adsorbed on the upper phosphorus compound layer, resulting in a reduction in heavy metals in the semiconductor substrate and a longer lifetime. A method using this Ringetter effect will be specifically explained with reference to FIGS. 1a to 1d.
What is shown in FIGS. 1a to 1d is an example of the manufacturing process of a thyristor, which is one of the individual elements. First, for example, Ga is diffused from both sides of an n-type Si substrate 11 to form a p-type layer 12 that will become an anode layer, and later a gate electrode is formed.
A p-type layer 13 serving as a base layer is formed to form a p-n-
A p-structure Si substrate 11 is obtained (FIG. 1a). Then p
A phosphorus glass layer 14 is formed on the p-type layer 13 serving as a base layer.
(deposition) (FIG. 1b). When this phosphorus glass layer 14 is formed, heavy metals contained in the Si substrate and heavy metals present outside are adsorbed to the phosphorus glass layer 14 . Thereafter, the phosphorus glass layer 14 is removed, and phosphorus contained near the surface of the Si substrate 11 is diffused to form an n-type layer 15 that will become a cathode layer (FIG. 1c). Note that the reason why phosphorus is diffused after removing the phosphorus glass layer 14 in this step is to control the surface concentration and depth of the n-type layer that will become the cathode layer. Thereafter, lifetime killer atoms (indicated by dots in the figure) are diffused from the side of the p-type layer 12, which will become the anode layer (FIG. 1d).
Finally, although not shown, the p layer 1 becomes the anode layer.
2 has an anode electrode and a p-type layer 13 which becomes a p base layer.
A thyristor element is obtained by forming a gate electrode and a cathode electrode on the n-type layer 15 which becomes a cathode layer. Since the thyristor element obtained in this way utilizes the Ringetter effect, the Si substrate 11
The amount of heavy metals inside is reduced and the life time is improved. However, the improvement in lifetime is due to
The amount is small, and as a result, it is almost the same as a thyristor using a method that does not use the Ringetter effect. A possible reason for this is that the phosphorus glass layer 14 is not formed when phosphorus is diffused, so the heavy metals attracted near the surface of the Si substrate 11 are
This is because when phosphorus is diffused, it is re-diffused and penetrates into the Si substrate 11. As described above, there was a fatal flaw in the manufacturing process in that while the lifetime was once increased during the formation (deposition) of the phosphorus glass layer, the carrier lifetime was lowered during the diffusion of phosphorus. The present invention was made in view of the above-mentioned drawbacks.
The present invention provides a method for manufacturing a semiconductor device with a high carrier lifetime and improved various characteristics. That is, the present invention diffuses phosphorus (n-type impurity) into a semiconductor substrate, and then forms a thin film having a thickness that allows phosphorus to pass through at least one surface of the semiconductor substrate and prevents phosphorus from being diffused into the semiconductor substrate. In this method, the semiconductor substrate is then heat-treated in an atmosphere containing phosphorus to improve the lifetime again. An embodiment of the present invention will be described below with reference to the drawings. FIGS. 2a to 2e show an embodiment of the present invention,
FIG. 2 is a process cross-sectional view showing the manufacturing process of the thyristor corresponding to FIG. 1; The steps a to c in FIG. 2 are the same as a to c in FIG. 1. That is, first, Ga is diffused from both sides of an n-type Si substrate 11 to form a p-type layer 12 that will become an anode layer, and a p-type layer 13 that will later become a p-base layer on which a gate electrode will be formed. Structure of Si
A substrate 11 is obtained (FIG. 2a). Next, a phosphorus glass layer 14 is formed (deposited) on the p-type layer 13, which becomes the p-base layer (FIG. 2b). At this time, the p-type layer 12 side, which normally becomes the anode layer, is not shown.
Cover with SiO 2 film, etc. This phosphorus glass layer 1
4, heavy metals contained in the Si substrate and heavy metals present outside are adsorbed to the phosphorus glass layer 14. Therefore, in this step, the lifetime of the Si substrate, especially the p-type layer which becomes the p-base layer, is improved several tens of times as will be explained later. After that, the phosphor glass layer 14 is removed, and the Si substrate 1 is
Phosphorus contained in 1 is diffused at a temperature of about 1200°C for about 5 hours to form an n-type layer 15 that will become a cathode layer (second
Figure c). In this step of diffusing phosphorus, as mentioned in the conventional example, the heavy metals that have been attracted near the surface of the Si substrate are re-diffused into the Si substrate, and the life tom of the Si substrate, especially the p-type layer 13 which becomes the p-base layer, is reduced. As will be explained later (FIG. 5), it returns to its original value.
The process up to this point is the same as the conventional method, that is, the method shown in FIG. The following step is an important step of the present invention. That is, after phosphorus is diffused into the p-type layer 13 of the Si substrate, which becomes the so-called p-base layer, a thermal oxide film 26 having a thickness that allows phosphorus to pass through and prevents phosphorus from being diffused into the substrate is applied to the p-type layer 12, which becomes the anode layer. This is a step of forming a substrate and heat-treating it in an atmosphere containing phosphorus (FIG. 2d). For example, a thermal oxide film 26 of 5000 Å is formed in an atmosphere containing phosphorus.
Heat treatment is performed at 1000°C for 1 hour. Here, the thermal oxide film is formed only on the p-type layer 12 which becomes the anode layer, but there is of course no problem in forming it on the n-type layer 15 which becomes the cathode layer. For example, in a semiconductor device such as a planar type device in which a p-type layer is exposed on the surface, a thermal oxide film should be formed on both surfaces to prevent phosphorus from diffusing into the semiconductor substrate. When the silicon substrate 11 is treated in an atmosphere containing phosphorus in this way, the lifetime, which had been lowered due to the phosphorus diffusion process, is improved again, and as will be explained later (Figure 5), the lifetime is improved by several tens of times immediately after the phosphorus diffusion process. do. Thereafter, the thermal oxide film 26 is removed, and Au atoms (indicated by dots in the figure), which are lifetime killer atoms, are diffused from the p-type layer 12 side, which will become the anode layer, in the same manner as in the step of FIG. 1d. Finally, although not shown, as in the conventional example, an anode electrode is formed on the p-type layer 12 that becomes the anode layer, a gate electrode is formed on the p-type layer 13 that becomes the p-base layer, and a cathode electrode is formed on the n-type layer 15 that becomes the cathode layer. As a result, a thyristor element can be obtained. FIGS. 3a to 3e are process sectional views showing other embodiments of the present invention and showing the manufacturing process of a thyristor corresponding to FIG. 1. The steps a to c in FIG. 3 are the same as a to c in FIG. 1. That is, first, Ga is diffused from both sides of an n-type Si substrate 11 to form a p-type layer 12 that will become an anode layer, and a p-type layer 13 that will later become a p-base layer on which a gate electrode will be formed to form a p-n-p structure. A Si substrate 11 of (FIG. 3a) is obtained. Next, a phosphorus glass layer 14 is formed (deposited) on the p-type layer 13, which becomes the p-base layer (FIG. 3b). At this time, the p-type layer 12 side, which normally becomes the anode layer, is not shown.
Cover with SiO 2 film, etc. This phosphorus glass layer 1
4, heavy metals contained in the Si substrate and heavy metals present outside are adsorbed to the phosphorus glass layer 14. Therefore, in this step, the lifetime of the Si substrate, especially the p-type layer which becomes the p-base layer, is improved several tens of times as will be explained later. After that, the phosphor glass layer 14 is removed, and the Si substrate 1 is
Phosphorus contained in 1 is diffused at a temperature of about 1200°C for about 5 hours to form an n-type layer 15 that will become a cathode layer (3rd layer).
Figure c). In this step of diffusing phosphorus, as mentioned in the conventional example, the heavy metals that were attracted near the surface of the Si substrate are re-diffused into the Si substrate, reducing the lifetime of the Si substrate, especially the p-type layer 13 which becomes the p-base layer. , it returns to its original value as will be explained later (FIG. 5). The process up to this point is the same as the conventional method, that is, the method shown in FIG. The following step is an important step of the present invention. In other words, a p-type layer 13 that becomes a so-called p base layer with phosphorus as a Si substrate.
This is a step of forming a low-temperature oxide film 37 on the p-type layer 12, which will become the anode layer, and having a thickness that allows phosphorus to pass through and prevents phosphorus from being diffused into the substrate, and then heat-treating this in an atmosphere containing phosphorus ( Figure 3 d).
For example, the low temperature oxide film 37 is formed using CVD method etc.
A film with a thickness of 5000 Å is formed and heat treated at 1000° C. for 1 hour in an atmosphere containing phosphorus. Here, the low-temperature oxide film is formed only on the p-type layer 12, which becomes the anode layer, but there is, of course, no problem in forming it on the n-type layer 15, which becomes the cathode layer. In a semiconductor device in which a mold layer is exposed, a low-temperature oxide film should be formed on both sides in order to prevent phosphorus from diffusing into the semiconductor substrate. When the silicon substrate 11 is treated in an atmosphere containing phosphorus in this way, the lifetime, which had decreased due to the phosphorus diffusion process, is improved again, as will be explained later (FIG. 5).
As a result, the improvement is several tens of times higher than that immediately after phosphorus diffusion. Thereafter, the low-temperature oxide film 37 is removed, and Au atoms (indicated by dots in the figure), which are lifetime killer atoms, are diffused from the p-type layer 12 side, which will become the anode layer, in the same manner as in the step shown in FIG. 1d. Finally, although not shown, as in the conventional example, an anode electrode is placed on the p-type layer 12 that becomes an anode layer, a gate electrode is placed on the p-type layer 13 that becomes a p-base layer,
A thyristor element is obtained by forming a cathode electrode on the n-type layer 15 serving as a cathode layer. FIGS. 4a to 4e show other embodiments of the present invention,
FIG. 2 is a process cross-sectional view showing the manufacturing process of the thyristor corresponding to FIG. 1; Items a to c in FIG. 4 are the same as a to c in FIG. 1. That is, first, the n-type Si substrate 11
Ga is diffused from both sides to form a p-type layer 12 that will become an anode layer, and a p-type layer 13 that will later become a p-base layer on which a gate electrode will be formed.
A substrate 11 is obtained (FIG. 4a). Next, a phosphorus glass layer 14 is formed (deposited) on the p-type layer 13, which will become the p-base layer (FIG. 4b).At this time, the p-type layer 12 side, which will become the anode layer, is usually SiO 2 (not shown).
Cover with a membrane, etc. When this phosphorus glass layer 14 is formed, heavy metals contained in the Si substrate and heavy metals present outside are adsorbed to the phosphorus glass layer 14 . Therefore, in this step, the lifetime of the Si substrate, especially the p-type layer which becomes the p-base layer, is improved several tens of times as will be explained later. Thereafter, the phosphorus glass layer 14 is removed, and the phosphorus contained in the Si substrate 11 is diffused at a temperature of about 1200° C. for about 5 hours to form an n-type layer 15 that will become a cathode layer (FIG. 4c).
In the process of diffusing this phosphorus, as described in the conventional example,
The heavy metals that had been attracted near the surface of the Si substrate are re-diffused into the Si substrate, and the P
The lifetime of the mold layer 13 decreases and returns to its original value as will be explained later (FIG. 3). The process up to this point is the same as the conventional method, that is, the method shown in FIG. The next step is an important step of the present invention. That is, phosphorus is Si
After diffusing into the p-type layer 13 which will become the so-called p-base layer of the substrate, a polycrystalline silicon film 48 having a thickness that allows phosphorus to pass therethrough and prevents phosphorus from being diffused into the substrate is formed on the p-type layer 12 which will become the anode layer. This is a process of heat-treating the material in an atmosphere containing phosphorus (Fig. 2d). Although it is assumed here that the polycrystalline silicon film is formed only on the p-type layer 12 that will become the anode layer, there is of course no problem in forming it on the n-type layer 15 that will become the cathode layer. Naturally, in a semiconductor device in which the p-type layer is exposed, polycrystalline silicon films should be formed on both sides in order to prevent phosphorus from diffusing into the semiconductor substrate. When the silicon substrate 11 is treated in an atmosphere containing phosphorus in this way, the lifetime, which had been lowered during the phosphorus diffusion process, is improved again, and as will be explained later (Figure 3), it is improved by several tens of times immediately after the phosphorus diffusion. . After that, the polycrystalline silicon film 48 is removed, and Au atoms (indicated by dots in the figure), which are lifetime killer atoms, are added from the p-type layer 12 side, which will become the anode layer, in the same manner as in the step d in FIG.
to spread. Finally, although not shown, an anode electrode is provided on the p-type layer 12 which becomes an anode layer as in the conventional example.
A thyristor element is obtained by forming a gate electrode on the p-type layer 13 serving as a p-base layer and forming a cathode electrode on the n-type layer 15 serving as a cathode layer. The thyristor element thus obtained is different from the conventional thyristor element obtained as shown in FIGS.
The mold layer has a long lifetime and good switching characteristics. Next, the lifetime of the p-type layer 13 which becomes the Si substrate, that is, the p base layer, of the thyristor element obtained as in the above example is compared with the lifetime of the p-type layer 13 which becomes the Si substrate, that is, the p base layer, of the thyristor element obtained in the conventional manner, that is, as shown in FIGS. p to be the base layer
How good the lifetime of the mold layer 13 is is specifically explained using the example shown in FIG. 2 with reference to FIG. 5. This figure 5 is different from the conventional figure 1 a.
- d and corresponding to Figs. 2 a to e of one embodiment of the present invention.
Lifetime (μsec) of the n-type layer 11 which becomes the n-base layer of the thyristor element for a′ to d′, a″ to e″
In this curve diagram, the dotted line is for the conventional case, and the solid line is for the embodiment of the present invention. As is clear from FIG. 5, in the conventional case, the life time of the n-type layer which is the n-base layer of the Si substrate is about 0.6 to 1.1 μsec, while in the case of the embodiment of the present invention, the life time of the n-type layer is about 0.6 to 1.1 μsec. The lifetime was about 1.1 to 1.3 μsec. That is, in the conventional case, there were many cases where the target value of 1.2 μsec. was not met, and the variation was large. On the other hand, in the case of one embodiment of the present invention, the target value was almost achieved and there was little variation. The reason why the lifetime almost achieved the target value and had little variation (good reproducibility) is that the silicon semiconductor substrate 11, which was masked with a thin film that transmits phosphorus again after diffusing phosphorus, as described above, By heat treatment in an atmosphere containing phosphorus, Si
The heavy metals re-diffused into the substrate and the external heavy metals are again adsorbed by the phosphorus in the atmosphere, and after this
This is because even if gold diffusion is performed at a temperature of about 850°C, the amount of heavy metals in the Si substrate will be reduced immediately after phosphorus is diffused. The measurement of lifetime in FIG. 5 was carried out by the diode voltage drop method, and what is shown in FIG. 5 is the change in lifetime when a heat treatment step of 700° C. was performed. In this way, the lifetime of the n-type layer, which becomes the n-base layer, is almost the target value, but unfortunately there is currently no means to directly measure the lifetime of the p-type layer 13, which becomes the p-base layer. This can be sufficiently determined by calculating the lifetime of the layer or by analogy with the device characteristics. Frequently used calculation formulas are
【式】で、τPB(X)はp型層の
深さの関数であるライフタイム、τNBはn型層1
1のライフタイム、CNBはn型層11の不純物濃
度、CPB(X)はp型層13の深さの関数である不
純物濃度を各々表わす。p型層の平均的なライフ
タイムPBはIn [Formula], τ PB(X) is the lifetime which is a function of the depth of the p-type layer, and τ NB is the lifetime of the n-type layer 1
1, CNB represents the impurity concentration of the n-type layer 11, and CPB (X) represents the impurity concentration as a function of the depth of the p-type layer 13, respectively. The average lifetime PB of the p-type layer is
【式】を用いれば簡単
に見積れる。ここでPBはp型層の平均不純物で
ある。
第5図に示した実験に用いた試料はCNB=4×
1013cm-3・PB=4×1017cm-3であるからPB=
τNB/100となるから、第5図に示すn型層のラ
イフタイムを1/100にすればp型層のライフタ
イムが得られる。ただし、金拡散工程におけるラ
イフタイムは、上記の関係式を用いることはでき
ず、選択的に金拡散されるn型層のライフタイム
は前工程より下がるが、金拡散の影響が殆ど及ば
ないp型層のライフタイムは前工程の値が殆ど維
持されることになる。
従つて第5図によれば、本発明のp型層ライフ
タイムは従来例に比べて約40倍もの大きさにな
る。なお本発明のリンを含む雰囲気での熱処理温
度はリンのゲツター効果を考慮すると700−1200
℃の範囲が適当である。
第6図にサイリスタの順方向阻止特性を従来a
と本発明の一実施例bとを比較して示し、第7図
に順方向導通特性を同様に従来aと本発明の一実
施例とを比較して示す。このうち第6図からは順
方向阻止電圧が本発明の一実施例の方法が従来
(第1図)方法に比べ、約2倍増加することが判
り、第7図からはアノード電流1000Aでのオン電
圧が約1/2に減少していることが判る。以上説明
したように本発明によれば、スイツチング特性
(時間的)を少し良く(複数個並列接続した場合
は上記したような作用効果がある)し、高耐圧化
及び低熱損失化が可能となり、さらに製造工程に
おける再現性と制御範囲が改善される。
以上第2図の実施例を用いて説明したが第3
図、第4図の実施例においても同様である。
なお、上記実施例において、サイリスタに適用
したが、本発明の方法はトランジスタ、GTO或
いは光サイリスタ等の固別素子、またバイポーラ
IC等のバイポーラ半導体素子に適用できること
は勿論である。また上記実施例において、金拡散
前の熱処理工程で代表的なものだけを考えたが、
本発明の方法は、リン拡散工程とライフタイムキ
ラー拡散工程との間に、熱酸化工程、p型拡散工
程、CVD工程等何等かの熱処理工程が介在して
も本発明の作用効果は損われない。
さらに上記実施例において、金拡散を施したサ
イリスタについて適用したが、金拡散を施さない
バイポーラ半導体素子についても同様に適用でき
る。It can be easily estimated using [Formula]. Here, PB is the average impurity of the p-type layer. The sample used in the experiment shown in Figure 5 was C NB =4×
10 13 cm -3・PB = 4×10 17 cm -3 , so PB =
Since τ NB /100, the lifetime of the p-type layer can be obtained by reducing the lifetime of the n-type layer shown in FIG. 5 to 1/100. However, the above relational expression cannot be used for the lifetime in the gold diffusion process, and the lifetime of the n-type layer in which gold is selectively diffused is lower than that in the previous process, but the p-type layer, which is hardly affected by gold diffusion, is As for the lifetime of the mold layer, most of the values from the previous process are maintained. Therefore, according to FIG. 5, the p-type layer lifetime of the present invention is about 40 times longer than that of the conventional example. In addition, the heat treatment temperature in the atmosphere containing phosphorus in the present invention is 700-1200, considering the getter effect of phosphorus.
A range of ℃ is suitable. Figure 6 shows the forward blocking characteristics of the thyristor in the conventional a
FIG. 7 shows a comparison of the forward conduction characteristics between conventional a and one embodiment of the present invention. From FIG. 6, it can be seen that the forward blocking voltage of the method according to the embodiment of the present invention is approximately twice as high as that of the conventional method (FIG. 1), and from FIG. It can be seen that the on-voltage is reduced by about 1/2. As explained above, according to the present invention, the switching characteristics (temporal) are slightly improved (when multiple devices are connected in parallel, the above-mentioned effects are obtained), and it is possible to increase the withstand voltage and reduce heat loss. Furthermore, reproducibility and control range in the manufacturing process are improved. The above explanation has been made using the embodiment shown in FIG.
The same applies to the embodiments shown in FIGS. Although the method of the present invention was applied to a thyristor in the above embodiment, it can also be applied to solid elements such as transistors, GTOs, or optical thyristors, as well as bipolar devices.
Of course, it can be applied to bipolar semiconductor devices such as ICs. In addition, in the above examples, only typical heat treatment steps before gold diffusion were considered;
In the method of the present invention, even if some heat treatment process such as a thermal oxidation process, a p-type diffusion process, or a CVD process is interposed between the phosphorus diffusion process and the lifetime killer diffusion process, the effects of the present invention are not impaired. do not have. Further, in the above embodiments, the present invention is applied to a thyristor with gold diffusion, but the present invention can be similarly applied to a bipolar semiconductor element without gold diffusion.
第1図a〜dは従来のスイツチング素子の製造
方法を説明するための工程断面図、第2図a〜e
は本発明の一実施例を説明するための工程断面
図、第3図a〜e及び第4図a〜eは本発明の他
の実施を説明するための工程断面図、第5図は第
1図の製造工程に対応したライフタイムの変化と
第2図の製造工程に対応したライフタイムの変化
とを対比して示した曲線図、第6図は本発明の一
実施例(第2図)の順方向阻止特性bと従来(第
1図)の順方向阻止特性aを対比して示した図、
第7図は本発明の一実施例(第2図)の順方向導
通特性と従来(第1図)の順方向導通特性を対比
して示した図である。
11……n型Si基体、11……Si基体、12…
…アノード層となるp型層、13……pベース層
となるp型層、14……リンガラス層、15……
カソード層となるn型層、26……熱酸化膜、3
7……低温酸化膜、48……多結晶シリコン膜。
Figures 1 a to d are process cross-sectional views for explaining a conventional method of manufacturing a switching element, and Figures 2 a to e
3A-3E and 4A-E are process sectional views for explaining another embodiment of the present invention, and FIG. 5 is a process sectional view for explaining another embodiment of the present invention. FIG. 6 is a curve diagram showing a comparison of changes in lifetime corresponding to the manufacturing process shown in FIG. 1 and changes in lifetime corresponding to the manufacturing process shown in FIG. A diagram comparing the forward blocking characteristic b of ) and the forward blocking characteristic a of the conventional (Fig. 1),
FIG. 7 is a diagram comparing the forward conduction characteristics of an embodiment of the present invention (FIG. 2) with the forward conduction characteristics of the conventional device (FIG. 1). 11... n-type Si substrate, 11... Si substrate, 12...
... p-type layer which becomes an anode layer, 13 ... p-type layer which becomes p base layer, 14 ... phosphorus glass layer, 15 ...
n-type layer serving as a cathode layer, 26...thermal oxide film, 3
7...Low temperature oxide film, 48...Polycrystalline silicon film.
Claims (1)
板の少なくとも一方の面にリンを透過し且つ前記
基体にリンが拡散されない厚さの薄膜を形成する
工程と、該工程により得られた半導体基体の両面
からリンを含む雰囲気中で熱処理する工程と、該
工程終了後前記薄膜の一部あるいは全部を除去す
る工程とを備えたことを特徴とする半導体素子の
製造方法。 2 半導体基体の少なくとも一方の面に形成する
薄膜が熱酸化膜であることを特徴とする特許請求
の範囲第1項記載の半導体素子の製造方法。 3 半導体基体の少なくとも一方の面に形成する
薄膜が低温酸化膜であることを特徴とする特許請
求の範囲第1項記載の半導体素子の製造方法。 4 半導体基体の少なくとも一方の面に形成する
薄膜が多結晶シリコン膜であることを特徴とする
特許請求の範囲第1項記載の半導体素子の製造方
法。 5 前記リンの熱処理工程の温度が700〜1200℃
であることを特徴とする特許請求の範囲第1項記
載の半導体素子の製造方法。[Claims] 1. A step of forming a thin film on at least one surface of a semiconductor substrate having at least one pn junction to a thickness that allows phosphorus to pass therethrough and prevents phosphorus from being diffused into the substrate, and 1. A method for manufacturing a semiconductor device, comprising the steps of heat-treating both sides of a semiconductor substrate in an atmosphere containing phosphorus, and removing part or all of the thin film after the step. 2. The method of manufacturing a semiconductor device according to claim 1, wherein the thin film formed on at least one surface of the semiconductor substrate is a thermal oxide film. 3. The method of manufacturing a semiconductor device according to claim 1, wherein the thin film formed on at least one surface of the semiconductor substrate is a low-temperature oxide film. 4. The method of manufacturing a semiconductor device according to claim 1, wherein the thin film formed on at least one surface of the semiconductor substrate is a polycrystalline silicon film. 5 The temperature of the phosphorus heat treatment step is 700 to 1200°C
A method for manufacturing a semiconductor device according to claim 1, characterized in that:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15430979A JPS5678128A (en) | 1979-11-30 | 1979-11-30 | Manufacture of semiconductor element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15430979A JPS5678128A (en) | 1979-11-30 | 1979-11-30 | Manufacture of semiconductor element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5678128A JPS5678128A (en) | 1981-06-26 |
| JPS6119104B2 true JPS6119104B2 (en) | 1986-05-15 |
Family
ID=15581292
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP15430979A Granted JPS5678128A (en) | 1979-11-30 | 1979-11-30 | Manufacture of semiconductor element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5678128A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0178703U (en) * | 1987-11-17 | 1989-05-26 | ||
| JPH05346102A (en) * | 1992-06-11 | 1993-12-27 | Sailor Pen Co Ltd:The | Control method for vertical air cylinder |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP4826993B2 (en) * | 2004-04-22 | 2011-11-30 | 信越半導体株式会社 | Method for producing p-type silicon single crystal wafer |
-
1979
- 1979-11-30 JP JP15430979A patent/JPS5678128A/en active Granted
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0178703U (en) * | 1987-11-17 | 1989-05-26 | ||
| JPH05346102A (en) * | 1992-06-11 | 1993-12-27 | Sailor Pen Co Ltd:The | Control method for vertical air cylinder |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5678128A (en) | 1981-06-26 |
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