JPH0249734Y2 - - Google Patents
Info
- Publication number
- JPH0249734Y2 JPH0249734Y2 JP648186U JP648186U JPH0249734Y2 JP H0249734 Y2 JPH0249734 Y2 JP H0249734Y2 JP 648186 U JP648186 U JP 648186U JP 648186 U JP648186 U JP 648186U JP H0249734 Y2 JPH0249734 Y2 JP H0249734Y2
- Authority
- JP
- Japan
- Prior art keywords
- gate
- buried gate
- layer
- buried
- electrodes
- 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
- 239000012535 impurity Substances 0.000 claims description 13
- 230000006698 induction Effects 0.000 claims description 9
- 230000003068 static effect Effects 0.000 claims description 8
- 230000002093 peripheral effect Effects 0.000 claims description 4
- 229910052751 metal Inorganic materials 0.000 description 4
- 239000002184 metal Substances 0.000 description 4
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 3
- 229910052796 boron Inorganic materials 0.000 description 3
- 239000004065 semiconductor Substances 0.000 description 3
- 230000003321 amplification Effects 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 230000008021 deposition Effects 0.000 description 2
- 229910052732 germanium Inorganic materials 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- 150000002739 metals Chemical class 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 238000003199 nucleic acid amplification method Methods 0.000 description 2
- 229910052710 silicon Inorganic materials 0.000 description 2
- GYHNNYVSQQEPJS-UHFFFAOYSA-N Gallium Chemical compound [Ga] GYHNNYVSQQEPJS-UHFFFAOYSA-N 0.000 description 1
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 1
- 239000000370 acceptor Substances 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 230000003111 delayed effect Effects 0.000 description 1
- 238000009792 diffusion process Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 229910052733 gallium Inorganic materials 0.000 description 1
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical compound [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000010703 silicon Substances 0.000 description 1
Landscapes
- Junction Field-Effect Transistors (AREA)
Description
〈産業上の利用分野〉
本考案は2個のゲート電極間を分割してそれぞ
れに不純物の異なる半導体材料を埋め込んだ埋込
ゲート型静電誘導型トランジスタに関する。
〈従来の技術〉
静電誘導型トランジスタ(以下SITと略す)は
大電力用,高耐圧用に適したゲートが埋込まれた
埋込ゲート型と小電力用,高速用に適したゲート
とソースとをほぼ同一平面上に形成された表面配
線型とに分類されている。
従来埋込ゲートのSITは第2図の構造概要の平
面図に示すように一般的に硅素Si,ゲルマニユー
ムGeなどの第族の真性半導体に、ほう素B,
アルミニユームAl,ガリウムGaなどの第族元
素をアクセプタとして拡散し、ゲート周縁部7の
両端に給電点としてゲート電極メタル6,6′を
配設している。このゲート周縁部7内にドレイン
N-とソースN層3の間に埋込ゲートP+層2より
なる第1埋込ゲート4を埋込んでSITが形成され
ている。
〈考案が解決しようとする問題点〉
従来の埋込ゲート型SITにおいては第1埋込ゲ
ート4の比較的に大きなゲート抵抗によつて給電
点であるゲート電極メタル6,6′より離れた部
分ではゲートの応答が近い部分より遅れるので、
1MHzを超える周波数における使用は困難であつ
た。
〈問題点を解決するための手段〉
ソースN層3とドレインN-1との間を結ぶ方
向に直交して設けられた埋込ゲートP+層2を囲
むゲート周辺部7の両端に設けゲート電極6,
6′を給電点とする埋込ゲート型静電誘導型トラ
ンジスタにおいて、埋込ゲートP+層2のゲート
電極6,6′に近くの第1埋込ゲートより第2埋
込ゲートの不純物密度を大とする静電誘導型トラ
ンジスタである。
〈作用〉
埋込ゲートの中央部分の不純物密度を高くして
ゲート抵抗の値を小さくして使用周波数が高くな
る。
〈実施例〉
本考案の埋込ゲート型静電誘導型トランジスタ
の実施例を図面を参照して説明する。
第1図に示すように上面のソースN層3とドレ
インN-層1との中間に埋め込まれた埋込ゲート
P+層2をその周縁に設けられたゲート周縁部7
の両端に給電点として設けられたゲート電極メタ
ル6,6′の間を給電点に近い第1埋込ゲート4
領域と中間の遠い第2埋込ゲート5領域に分割し
て形成する。これら分割された第1埋込ゲート4
領域における不純物密度より第2埋込ゲート5領
域の不純物密度を大きくするものである。ここに
おける不純物密度とは実用化されているように真
性半導体Siに対し第族元素Bを不純物として混
ぜたときの1cm3あたりの原子数の割合をいう。
いま具体的の例として第1埋込ゲート4の長さ
3mm,第2埋込ゲート5の長さ4mmに対しドレイ
ンN-層1の不純物密度ND=5×1013cm-3,ソー
スN層3の不純物密度Nd=1×1015cm-3である。
これに対し第1埋込ゲート4の密度と第2埋込ゲ
ート5の密度を従来例と本考案によるサンプル6
個についてそれぞれのデータと電圧増幅率μが
3dB低下する周波数fT(MHz)を比較測定した値
は第1表に示す。
<Industrial Application Field> The present invention relates to a buried gate static induction transistor in which the space between two gate electrodes is divided and semiconductor materials with different impurities are embedded in each of the gate electrodes. <Conventional technology> Static induction transistors (hereinafter abbreviated as SIT) have two types: a buried gate type suitable for high power and high voltage applications, and a gate and source type suitable for low power and high speed applications. and surface wiring type, which are formed on almost the same plane. As shown in the plan view of the structural outline in Figure 2, the conventional buried gate SIT generally uses a group of intrinsic semiconductors such as silicon Si and germanium Ge, as well as boron B,
Group group elements such as aluminum Al and gallium Ga are diffused as acceptors, and gate electrode metals 6 and 6' are provided at both ends of the gate peripheral portion 7 as power feeding points. A drain is placed within this gate peripheral portion 7.
A SIT is formed by embedding a first buried gate 4 made of a buried gate P + layer 2 between the N − and source N layers 3 . <Problems to be solved by the invention> In the conventional buried gate type SIT, due to the relatively large gate resistance of the first buried gate 4, the portion away from the gate electrode metal 6, 6' which is the power supply point In this case, the response of the gate is delayed compared to the nearby part, so
It was difficult to use it at frequencies exceeding 1MHz. <Means for solving the problem> A buried gate provided perpendicularly to the direction connecting the source N layer 3 and the drain N − 1 is provided at both ends of the gate peripheral portion 7 surrounding the buried gate P + layer 2. electrode 6,
In a buried gate static induction transistor with 6' as the power supply point, the impurity density of the second buried gate is lower than that of the first buried gate near the gate electrodes 6 and 6' of the buried gate P + layer 2. It is a static induction type transistor with a large size. <Operation> By increasing the impurity density in the central part of the buried gate, the value of gate resistance is reduced, and the operating frequency is increased. <Example> An example of the buried gate static induction transistor of the present invention will be described with reference to the drawings. As shown in Figure 1, a buried gate is buried between the source N layer 3 and the drain N - layer 1 on the upper surface.
Gate periphery 7 with P + layer 2 provided on its periphery
between the gate electrode metals 6 and 6' provided as a power supply point at both ends of the first buried gate 4 near the power supply point.
The second buried gate 5 is formed by dividing into a region and a second buried gate 5 region located far away in the middle. These divided first embedded gates 4
The impurity density in the second buried gate 5 region is made higher than the impurity density in the second buried gate 5 region. The impurity density here refers to the ratio of the number of atoms per 1 cm 3 when a group element B is mixed as an impurity to the intrinsic semiconductor Si, as is practically used. As a specific example, for a length of the first buried gate 4 of 3 mm and a length of the second buried gate 5 of 4 mm, the impurity density of the drain N -layer 1 is N D =5×10 13 cm -3 , and the source N The impurity density of layer 3 is N d =1×10 15 cm −3 .
On the other hand, the density of the first buried gate 4 and the density of the second buried gate 5 are different from that of the conventional example and the sample 6 according to the present invention.
The respective data and voltage amplification factor μ for each
Table 1 shows the comparatively measured values of the frequency f T (MHz) that decreases by 3 dB.
【表】
第1表より明らかなように第1埋込ゲート4の
密度Ns1=2または3×10-19cm-3,第2埋込ゲー
ト5の密度Ns2=2〜6×10-19cm-3においてNs2
を大きくすることによつて使用周波数は大きく改
善される。しかし現在1kWのSITに要求されるfT
は1.2MHz程度が生産可能な値である。
ここで不純物密度が異なるゲートを得る方法と
して、第1埋込ゲート4と第2埋込ゲート5を
別々に選択拡散を行なうか、またはまず高い不純
物密度の条件で全ゲートパタンにプレデポジシヨ
ンを施しておき、その後第1埋込ゲート4領域の
みプレデポジシヨンで形成されたボロンガラスを
一部除去し、しかる後全体を高温加熱する,いわ
ゆるドライブインを施す。なお本実施例において
は第1埋込ゲート4と第2埋込ゲート5との不純
物密度比は1:3であるが第1埋込ゲート4のボ
ロンガラスの除去量を加減することによつて更に
この比を変えることができる。
〈考案の効果〉
以上に述べたように本考案によれば、許容損失
1kW程度のSITにおいては電圧増幅率μの周波数
依存性は3dB低下時2.0MHzであり従来の0.8MHz
にくらべ大幅に改善される。したがつて素子の価
格,形状,電力値を変えることなく周波数特性の
改善が可能となる。[Table] As is clear from Table 1, the density of the first buried gate 4 is N s1 = 2 or 3×10 -19 cm -3 , and the density of the second buried gate 5 is N s2 = 2 to 6×10 - N s2 at 19 cm -3
By increasing , the frequency used can be greatly improved. However, currently f T required for 1kW SIT
The value that can be produced is about 1.2MHz. Here, as a method of obtaining gates with different impurity densities, selective diffusion is performed separately on the first buried gate 4 and the second buried gate 5, or pre-deposition is first performed on all gate patterns under conditions of high impurity density. Thereafter, a portion of the boron glass formed by pre-deposition is removed only in the first buried gate 4 area, and then the entire area is heated at a high temperature, ie, a so-called drive-in process is performed. In this embodiment, the impurity density ratio between the first buried gate 4 and the second buried gate 5 is 1:3, but it can be changed by adjusting the amount of boron glass removed from the first buried gate 4. Furthermore, this ratio can be varied. <Effects of the invention> As stated above, according to the invention, the allowable loss
In a SIT of about 1kW, the frequency dependence of the voltage amplification factor μ is 2.0MHz when it decreases by 3dB, compared to the conventional 0.8MHz.
It is significantly improved compared to . Therefore, it is possible to improve the frequency characteristics without changing the price, shape, or power value of the element.
第1図は本考案の静電誘導型トランジスタの実
施例でaは外観平面図,bはaにおけるA−A線
における縦断正面図,cはaにおけるB−B線に
おける縦断側面図,第2図は従来の静電誘導型ト
ランジスタの外観平面図である。
なお、1……ドレインN-層、2……埋込ゲー
トP+層、3……ソースN層、4……第1埋込ゲ
ート、5……第2埋込ゲート、6,6′……ゲー
ト電極メタル、7……ゲート周辺部。
FIG. 1 shows an embodiment of the static induction transistor of the present invention, in which a is an external plan view, b is a vertical front view taken along line A-A in a, c is a vertical side view taken along line B-B in a, and FIG. The figure is an external plan view of a conventional static induction transistor. Note that 1...Drain N - layer, 2...Buried gate P + layer, 3...Source N layer, 4...First buried gate, 5...Second buried gate, 6, 6'... ...Gate electrode metal, 7...Gate periphery.
Claims (1)
との間を結ぶ方向に直交して設けられた埋込ゲー
トP+層2を囲むゲート周辺部7の両端に給電点
としてゲート電極6,6′を設けた埋込ゲート型
静電誘導型トランジスタにおいて、前記ゲート電
極6,6′間の前記埋込ゲートP+層2の両電極に
対し近くより遠くが不純物密度を大としてなる静
電誘導型トランジスタ。 Source N layer 3 on the top surface and drain N - layer 1 on the bottom surface
A buried gate static induction type transistor in which gate electrodes 6 and 6' are provided as power feeding points at both ends of a gate peripheral area 7 surrounding a buried gate P + layer 2 provided perpendicular to the direction connecting between In the electrostatic induction type transistor, the impurity density is higher in the buried gate P + layer 2 between the gate electrodes 6 and 6' at a distance from both electrodes than near the electrodes.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP648186U JPH0249734Y2 (en) | 1986-01-22 | 1986-01-22 |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP648186U JPH0249734Y2 (en) | 1986-01-22 | 1986-01-22 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62120367U JPS62120367U (en) | 1987-07-30 |
| JPH0249734Y2 true JPH0249734Y2 (en) | 1990-12-27 |
Family
ID=30789032
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP648186U Expired JPH0249734Y2 (en) | 1986-01-22 | 1986-01-22 |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0249734Y2 (en) |
-
1986
- 1986-01-22 JP JP648186U patent/JPH0249734Y2/ja not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62120367U (en) | 1987-07-30 |
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