JPH045861A - Semiconductor device - Google Patents
Semiconductor deviceInfo
- Publication number
- JPH045861A JPH045861A JP10814390A JP10814390A JPH045861A JP H045861 A JPH045861 A JP H045861A JP 10814390 A JP10814390 A JP 10814390A JP 10814390 A JP10814390 A JP 10814390A JP H045861 A JPH045861 A JP H045861A
- Authority
- JP
- Japan
- Prior art keywords
- channel
- semiconductor device
- drain
- impurity
- field effect
- 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.)
- Pending
Links
Landscapes
- Insulated Gate Type Field-Effect Transistor (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は、半導体装置に関し、特に電界効果型トラン
ジスタの微細化に伴う短チヤネル効果の改善を図ったも
のに関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a semiconductor device, and particularly to a semiconductor device in which short channel effects associated with miniaturization of field effect transistors are improved.
第4図は従来の半導体装置である電界効果型トランジス
タを示す断面図であり、図において、1はソース電極、
2はバックゲート電極、3はゲート電極、4はゲート酸
化膜、5はドレイン電極、6はソース拡散層、7はドレ
イン拡散層、8は基板である。FIG. 4 is a cross-sectional view showing a field effect transistor, which is a conventional semiconductor device. In the figure, 1 is a source electrode;
2 is a back gate electrode, 3 is a gate electrode, 4 is a gate oxide film, 5 is a drain electrode, 6 is a source diffusion layer, 7 is a drain diffusion layer, and 8 is a substrate.
次に不純物分布について説明する。Next, impurity distribution will be explained.
第5図は電界効果型トランジスタの動作状態における電
流経路を示しており、9の領域はチャネルと呼ばれる。FIG. 5 shows a current path in the operating state of a field effect transistor, and the region 9 is called a channel.
このチャネル領域9はトランジスタの闇値電圧を制御す
るためにボロンやヒ素といった不純物イオンが10”/
c♂程度注入されている。これらの不純物イオンの注入
はイオン注入機を用いて電界効果トランジスタの上部空
間よりウェハに向かって行われるため、深さ方向に対し
ては分布を持つが、横方向(すなわち、ソース・ドレイ
ンを結ぶ直線に沿うチャネル方向)に対しては分布を持
たず均一となる。In order to control the dark voltage of the transistor, impurity ions such as boron and arsenic are added to this channel region 9 at a rate of 10"/
About c♂ has been injected. These impurity ions are implanted using an ion implanter from the space above the field effect transistor toward the wafer, so they have a distribution in the depth direction, but they have a distribution in the lateral direction (i.e., connecting the source and drain). In the direction of the channel (along a straight line), it has no distribution and is uniform.
従来の電界効果型トランジスタは以上のように構成され
ているので、この構造のまま0.3ミクロン程度まで微
細化するには、短チヤネル効果を抑える必要性から不純
物イオンの注入量を増し、ドレイン空乏層の伸びを抑え
なければならず、結局、ドレイン近傍での電界強度が強
くなり、ホットキャリア対策が必要になるという問題が
あった。Conventional field effect transistors have the structure described above, so in order to miniaturize the structure to about 0.3 microns, the amount of impurity ions implanted must be increased to suppress the short channel effect, and the drain The problem is that the growth of the depletion layer must be suppressed, and as a result, the electric field strength near the drain becomes stronger, making it necessary to take countermeasures against hot carriers.
この発明は上記のような問題点を解消するためになされ
たもので、短チヤネル効果を伴うことなく、微細化可能
な電界効果型トランジスタを有する半導体装置を得るこ
とを目的とする。The present invention has been made to solve the above-mentioned problems, and an object of the present invention is to obtain a semiconductor device having a field effect transistor that can be miniaturized without causing short channel effects.
この発明に係る半導体装置は、電界効果型トランジスタ
のチャネル領域での不純物イオンを横方向にも分布する
ようにしたものである。In the semiconductor device according to the present invention, impurity ions in the channel region of a field effect transistor are also distributed in the lateral direction.
この発明における半導体装置では、上述のようにチャネ
ル領域において、横方向に不純物イオンの分布を持たせ
たので、ドレイン近傍といった必要な領域のみ不純物濃
度を濃くすることができる。In the semiconductor device according to the present invention, since the impurity ions are distributed laterally in the channel region as described above, the impurity concentration can be increased only in a necessary region such as near the drain.
以下、この発明の一実施例を図について説明する。 An embodiment of the present invention will be described below with reference to the drawings.
第1図はこの発明の一実施例による半導体装置を示し、
図において、1はソース電極、2はバックゲート電極、
3はゲート電極、4はゲート酸化膜、5はドレイン電極
、6はソース拡散層、7はドレイン拡散層、8は基板で
ある。FIG. 1 shows a semiconductor device according to an embodiment of the present invention,
In the figure, 1 is a source electrode, 2 is a back gate electrode,
3 is a gate electrode, 4 is a gate oxide film, 5 is a drain electrode, 6 is a source diffusion layer, 7 is a drain diffusion layer, and 8 is a substrate.
第2図は第1図のx−x ’断面における不純物分布を
示す。なお、第2図ではnチャネル型の電界効果トラン
ジスタを想定した場合のチャネル方向の不純物分布であ
る。ここで、縦軸の濃度の値はデバイス構造によって変
わるため、濃度は最大不純物濃度で規格化している。FIG. 2 shows the impurity distribution in the xx' cross section of FIG. 1. Note that FIG. 2 shows the impurity distribution in the channel direction assuming an n-channel field effect transistor. Here, since the concentration value on the vertical axis varies depending on the device structure, the concentration is normalized by the maximum impurity concentration.
次にその製造方法について第3図を参照して説明する。Next, the manufacturing method will be explained with reference to FIG.
なお、ここでは従来の電界効果トランジスタの製造方法
と異なる工程となるチャネルドーズについてのみ説明す
る。Note that only the channel dose, which is a different step from the conventional method of manufacturing a field effect transistor, will be described here.
■ P型のシリコン基板8上に、0.1〜0゜2ミクロ
ンのソース・ドレイン拡散層深さ程度に不純物濃度のピ
ーク位置がくるようポロンといったP型の不純物をイオ
ン注入し、パンチスルーストッパとする。■ A P-type impurity such as poron is ion-implanted onto the P-type silicon substrate 8 so that the peak of the impurity concentration is at the depth of the source/drain diffusion layer of 0.1 to 0.2 microns to form a punch-through stopper. shall be.
■ レジストを付け、チャネル部を残して写真製版をす
る。■ Apply resist and photolithography leaving the channel area.
■ 斜めイオン注入を行う。■ Perform oblique ion implantation.
後は従来と同様のプロセスにより、ゲート酸化膜を形成
し、ゲートポリシリコンを取付けてパタニングを行なう
ことにより、本実施例の半導体装置が得られる。Thereafter, the semiconductor device of this example is obtained by forming a gate oxide film, attaching gate polysilicon, and performing patterning using the same process as in the prior art.
■の斜めイオン注入ではイオンの注入経路におけるレジ
スト膜厚の違いを利用する。レジスト膜厚が薄いと、イ
オンは突き抜ける。従って、第3図(C)の場合、レジ
スト下面の左側にはイオンが多く入ることになる。長チ
ャネルの電界効果トランジスタでは、レジストでイオン
が阻止されるため、ドレイン近傍で分布を持たせること
は不可能であるが、短チャネルの電界効果トランジスタ
では分布を持たせることが可能である。(2) Oblique ion implantation utilizes differences in resist film thickness along the ion implantation path. If the resist film is thin, ions can penetrate through it. Therefore, in the case of FIG. 3(C), many ions enter the left side of the lower surface of the resist. In a long channel field effect transistor, ions are blocked by the resist, so it is impossible to create a distribution near the drain, but in a short channel field effect transistor, it is possible to create a distribution.
このように、本実施例では斜め方向にイオン注入を行な
うことにより、チャネル部に横方向のプロファイルを持
たせ、ドレイン近傍での電界を緩和するようにしたので
、LDD構造のトランジスタに比し、極めて簡単のプロ
セスで、短チヤネル効果を防止できる効果がある。In this way, in this example, by performing ion implantation in an oblique direction, the channel part has a horizontal profile and the electric field near the drain is relaxed, so compared to a transistor with an LDD structure, This is an extremely simple process and is effective in preventing the short channel effect.
なお、上記実施例ではバソクゲ−1・電極2を素子下部
に取り付けたが、これは基板のP領域と短絡していれば
どこに取り付けてもよい。In the above embodiment, the electrode 1 and the electrode 2 are attached to the bottom of the element, but they may be attached anywhere as long as they are short-circuited to the P region of the substrate.
以上のように、この発明に係る半導体装置によれば、チ
ャネル領域の不純物分布を横方向にも持たせたので、ド
レイン近傍では選択的に濃度を薄くすることが可能で、
ドレイン近傍での電界強度を弱くすることができる。そ
の結果、衝突電離現象を低減させることができ、ホット
エレクトロン効果を抑えることができ、微細化に寄与で
きる。As described above, according to the semiconductor device according to the present invention, since the impurity distribution in the channel region is also provided in the lateral direction, it is possible to selectively reduce the concentration near the drain.
The electric field strength near the drain can be weakened. As a result, it is possible to reduce the impact ionization phenomenon, suppress the hot electron effect, and contribute to miniaturization.
第1図はこの発明の一実施例による半導体装置を示す断
面図、第2図はチャネルでの横方向不純物の分布を示す
特性図、第3図は本発明の一実施例による半導体装置の
製造工程を示すプロセスフロー図、第4図は従来の半導
体装置を示す断面図、第5図は従来の半導体装置の動作
状態における電流経路を示す図である。
図において、■はソース電極、2はバックゲート電極、
3はゲート電極、4はゲート酸化膜、5はドレイン電極
、6はソース拡散層、7はドレイン拡散層、8は基板、
9はチャネル、工0はチャネルを流れる電流経路である
。
なお図中同一符号は同−又は相当部分を示す。FIG. 1 is a cross-sectional view showing a semiconductor device according to an embodiment of the present invention, FIG. 2 is a characteristic diagram showing the distribution of lateral impurities in a channel, and FIG. 3 is a fabrication of a semiconductor device according to an embodiment of the present invention. FIG. 4 is a sectional view showing a conventional semiconductor device, and FIG. 5 is a diagram showing current paths in the operating state of the conventional semiconductor device. In the figure, ■ is the source electrode, 2 is the back gate electrode,
3 is a gate electrode, 4 is a gate oxide film, 5 is a drain electrode, 6 is a source diffusion layer, 7 is a drain diffusion layer, 8 is a substrate,
9 is a channel, and 0 is a current path flowing through the channel. Note that the same reference numerals in the figures indicate the same or equivalent parts.
Claims (1)
おいて、 チャネル領域における不純物分布をチャネル方向に変化
させたことを特徴とする半導体装置。(1) A semiconductor device constituting a field effect transistor, characterized in that the impurity distribution in the channel region is changed in the channel direction.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10814390A JPH045861A (en) | 1990-04-23 | 1990-04-23 | Semiconductor device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10814390A JPH045861A (en) | 1990-04-23 | 1990-04-23 | Semiconductor device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH045861A true JPH045861A (en) | 1992-01-09 |
Family
ID=14477029
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10814390A Pending JPH045861A (en) | 1990-04-23 | 1990-04-23 | Semiconductor device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH045861A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2003178995A (en) * | 2001-09-28 | 2003-06-27 | Agere Systems Guardian Corp | Ion implantation method to achieve desired dopant concentration |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5435682A (en) * | 1977-08-26 | 1979-03-15 | Agency Of Ind Science & Technol | Manufacture of field effect transistor |
| JPS62155565A (en) * | 1985-12-27 | 1987-07-10 | Toshiba Corp | Insulated-gate field effect transistor and manufacture thereof |
-
1990
- 1990-04-23 JP JP10814390A patent/JPH045861A/en active Pending
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5435682A (en) * | 1977-08-26 | 1979-03-15 | Agency Of Ind Science & Technol | Manufacture of field effect transistor |
| JPS62155565A (en) * | 1985-12-27 | 1987-07-10 | Toshiba Corp | Insulated-gate field effect transistor and manufacture thereof |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2003178995A (en) * | 2001-09-28 | 2003-06-27 | Agere Systems Guardian Corp | Ion implantation method to achieve desired dopant concentration |
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