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JPH0834312B2 - Vertical field effect transistor - Google Patents

Vertical field effect transistor

Info

Publication number
JPH0834312B2
JPH0834312B2 JP63308285A JP30828588A JPH0834312B2 JP H0834312 B2 JPH0834312 B2 JP H0834312B2 JP 63308285 A JP63308285 A JP 63308285A JP 30828588 A JP30828588 A JP 30828588A JP H0834312 B2 JPH0834312 B2 JP H0834312B2
Authority
JP
Japan
Prior art keywords
layer
gate
window
effect transistor
source layer
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 - Lifetime
Application number
JP63308285A
Other languages
Japanese (ja)
Other versions
JPH02154469A (en
Inventor
和広 土屋
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji 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 Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP63308285A priority Critical patent/JPH0834312B2/en
Priority to FR8916139A priority patent/FR2640081A1/en
Priority to DE3940388A priority patent/DE3940388A1/en
Publication of JPH02154469A publication Critical patent/JPH02154469A/en
Publication of JPH0834312B2 publication Critical patent/JPH0834312B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D12/00Bipolar devices controlled by the field effect, e.g. insulated-gate bipolar transistors [IGBT]
    • H10D12/411Insulated-gate bipolar transistors [IGBT]
    • H10D12/441Vertical IGBTs
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D62/00Semiconductor bodies, or regions thereof, of devices having potential barriers
    • H10D62/10Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
    • H10D62/124Shapes, relative sizes or dispositions of the regions of semiconductor bodies or of junctions between the regions
    • H10D62/126Top-view geometrical layouts of the regions or the junctions
    • H10D62/127Top-view geometrical layouts of the regions or the junctions of cellular field-effect devices, e.g. multicellular DMOS transistors or IGBTs
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D62/00Semiconductor bodies, or regions thereof, of devices having potential barriers
    • H10D62/10Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
    • H10D62/17Semiconductor regions connected to electrodes not carrying current to be rectified, amplified or switched, e.g. channel regions
    • H10D62/393Body regions of DMOS transistors or IGBTs 
    • H10P76/40

Landscapes

  • Insulated Gate Type Field-Effect Transistor (AREA)
  • Junction Field-Effect Transistors (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は個別素子や集積回路装置に組み込むに適する
DMOS(二重拡散MOS)の通称で知られている縦形電界効
果トランジスタに関する。
DETAILED DESCRIPTION OF THE INVENTION [Industrial field of application] The present invention is suitable for being incorporated into an individual element or an integrated circuit device.
The present invention relates to a vertical field effect transistor commonly known as DMOS (double diffused MOS).

〔従来の技術〕[Conventional technology]

縦形電界効果トランジスタは通常のMOSトランジスタ
のような横形構造のものと比較して高耐圧かつ大電流用
に適し、従来から主に高周波用のパワートランジスタと
して実用化され広範な用途で用いられている。この縦形
電界効果トランジスタは、集積回路技術を利用して作ら
れる微小トランジスタを多数個並列接続した構造をもつ
ので、上のパワートランジスタ等の個別素子に限らず、
負荷を直接駆動する集積回路装置への組み込み用にも適
する。第3図はこの代表的な従来例を示すもので、同図
(a)はその一部拡大平面図,同図(b)にはそのX−
X矢視断面図である。
Vertical field-effect transistors are suitable for high withstand voltage and large current compared to those with horizontal structure such as ordinary MOS transistors, and have been practically used as power transistors for high frequencies and have been used in a wide range of applications. . This vertical field-effect transistor has a structure in which a large number of microtransistors made by using integrated circuit technology are connected in parallel, so that the vertical field-effect transistor is not limited to the above-mentioned individual elements such as power transistors,
It is also suitable for incorporation into integrated circuit devices that drive loads directly. FIG. 3 shows this typical conventional example. FIG. 3 (a) is a partially enlarged plan view thereof, and FIG.
It is X sectional view taken on the arrow.

この例での縦形電界効果トランジスタは、個別素子用
のnチャネル形のものであって、第3図(b)のドレイ
ン層2は高不純物濃度の低抵抗性のn形とされ、その上
のエピタキシャル層等の半導体領域3もn形で、動作上
はこれがドレイン領域の役目を果たす。この半導体領域
3の表面をごく薄いゲート酸化膜4を介して覆うように
多結晶シリコン等のゲート5が設けられ、さらに同図
(a)に示すように、このゲート5にふつうは数〜10μ
m角程度の正方形の窓5bがこの例では正方配列で多数個
抜かれる。なお、この窓5bは六角形に形成されることも
あり、この場合には窓5bはその形状に応じて六方配列さ
れる。
The vertical field effect transistor in this example is an n-channel type for an individual device, and the drain layer 2 in FIG. 3 (b) is an n-type having a high impurity concentration and a low resistance, and is formed thereon. The semiconductor region 3 such as an epitaxial layer is also n-type and, in operation, this serves as a drain region. A gate 5 of polycrystalline silicon or the like is provided so as to cover the surface of the semiconductor region 3 with a very thin gate oxide film 4 interposed therebetween. Further, as shown in FIG.
In this example, a large number of square windows 5b of about m square are cut out in a square array. The window 5b may be formed in a hexagonal shape, and in this case, the windows 5b are hexagonally arranged according to the shape.

チャネル形成層6は、ゲート5をマスクとしてその窓
5bからイオン注入法を利用してp形で拡散され、その周
縁部がゲート5の下にもぐり込むように作り込まれる。
ついで、同様にゲート5をマスクするイオン注入法によ
り、強いn形のソース層7がチャネル形成層6よりは浅
くかつその周縁が僅かにゲート5の下にもぐり込むよう
に拡散される。さらに窓5bの中央部に、強いp形のコン
タクト層8が、同図(b)からわかるようにソース層7
を突き抜けてチャネル形成層6に達するように拡散され
る。以後は同図(b)に示すように、酸化膜等の絶縁膜
9がゲート5を覆うように設けられ、さらにその上にソ
ース電極10が窓5b内のソース層7およびコンタクト層8
の表面に導電接触するように設けられる。図の下側のド
レイン層2にはドレイン電極11が接続される。なお、同
図(a)は図示の都合上ソース電極10がない状態で示さ
れていることを留意されたい。
The channel formation layer 6 has its window with the gate 5 as a mask.
P-type diffusion is carried out from 5b using the ion implantation method, and the peripheral portion thereof is formed so as to dig under the gate 5.
Then, the strong n-type source layer 7 is diffused so that it is shallower than the channel forming layer 6 and its peripheral edge slightly goes under the gate 5 by the ion implantation method which also masks the gate 5. Further, a strong p-type contact layer 8 is formed at the center of the window 5b, as shown in FIG.
Is diffused to reach the channel formation layer 6 through the. After that, as shown in FIG. 3B, an insulating film 9 such as an oxide film is provided so as to cover the gate 5, and a source electrode 10 is further provided thereon to form a source layer 7 and a contact layer 8 in the window 5b.
To be in conductive contact with the surface of the. A drain electrode 11 is connected to the drain layer 2 on the lower side of the figure. It should be noted that FIG. 1A is shown without the source electrode 10 for convenience of illustration.

以上の構造をもつ縦形電界効果トランジスタでは、第
3図(b)に示すようにゲート5からゲート端子Gが,
ソース電極10からソース端子Sが,ドレイン電極11から
ドレイン端子Dがそれぞれ導出され、例えばドレイン端
子Dを正の電位に,ソース端子Sを接地電位にそれぞれ
置いた状態で使用される。ゲート端子Gに正の電圧が与
えられた時、ゲート5の下のp形のチャネル形成層6の
表面にn形のチャネルが形成され、図示のように多数キ
ャリアとしての電子eがn形のソース層7からこのnチ
ャネルを経てn形の半導体領域4に入り、この半導体領
域4内を縦方向に流れてn形のドレイン層2に至る。
In the vertical field effect transistor having the above structure, as shown in FIG. 3 (b), the gate 5 to the gate terminal G are
A source terminal S is led out from the source electrode 10 and a drain terminal D is led out from the drain electrode 11, respectively. For example, the drain terminal D is used at a positive potential and the source terminal S is placed at a ground potential. When a positive voltage is applied to the gate terminal G, an n-type channel is formed on the surface of the p-type channel forming layer 6 below the gate 5, and as shown in the figure, electrons e as majority carriers are n-type. The source layer 7 enters the n-type semiconductor region 4 through the n-channel, flows vertically in the semiconductor region 4, and reaches the n-type drain layer 2.

ソース層7とコンタクト層8はソース電極10により短
絡されており、これによってチャネル形成層6がソース
層7と実質上同電位に保たれて、この電界効果トランジ
スタのゲートしきい値が安定化される。オフ動作時に掛
かる電源電圧は、半導体領域4とチャネル形成層6との
間のpn接合から半導体領域4内に延びる空乏層によって
主に負担されるので、高耐圧値をこの縦形電界効果トラ
ンジスタに持たせることができる。また、電流容量は当
然そのチャネル幅すなわちソース層7の周辺流によって
決まるから、フォトプロセス精度から許される限り並列
接続する微小トランジスタのパターンを小形化して単位
チップ面積あたりのソース層7の周辺長の合計を増加さ
せることにより、その電流容量の向上ないしはオン抵抗
の減少が図られる。
The source layer 7 and the contact layer 8 are short-circuited by the source electrode 10, which keeps the channel forming layer 6 at substantially the same potential as the source layer 7 and stabilizes the gate threshold value of this field effect transistor. It Since the power supply voltage applied during the off operation is mainly borne by the depletion layer extending from the pn junction between the semiconductor region 4 and the channel forming layer 6 into the semiconductor region 4, the vertical field effect transistor has a high withstand voltage value. Can be made. Since the current capacity is naturally determined by the channel width, that is, the peripheral flow of the source layer 7, the pattern of the minute transistors connected in parallel is miniaturized to allow the peripheral length of the source layer 7 per unit chip area as long as the photoprocess accuracy allows. By increasing the total, the current capacity is improved or the on-resistance is reduced.

〔発明が解決しようとする課題〕[Problems to be Solved by the Invention]

上述のように縦形電界効果トランジスタではそれに掛
かる電圧は主には半導体領域4内で負担されるものの、
そのごく短いふつうは1〜2μm程度のチャネル長に過
電圧が掛かると、チャネルのいわゆるパンチスルーが発
生して制御不能になり、このパンチスルー電圧を向上し
ようとすると、電流容量の方が減少しやすい問題があ
る。
As described above, in the vertical field effect transistor, although the voltage applied to it is mainly borne in the semiconductor region 4,
If the overlength is applied to the channel length of about 1 to 2 μm, the so-called punch-through of the channel occurs and the control becomes uncontrollable, and if the punch-through voltage is improved, the current capacity tends to decrease. There's a problem.

上述のパンチスルーは第3図(a)からもわかるよう
に、チャネル形成層6およびソース層7の方形の拡散パ
ターンの角部に電界が集中するために発生しやすく、こ
の電界集中を極力緩和するため、例えば図では1個所に
のみ示された連絡層6aを隣合う4個のチャネル形成層6
の角部を相互に結合するようにX形で設けるなどの工夫
が従来からなされている。ところが、この角部に元来チ
ャネル電流が多く流れやすいこともあって、この手段で
は角部に流れる電流がなくなるから、ソース層7の有効
周辺長が減少して電流容量がかなり減少してしまう。ま
た、連絡層6aはもちろんゲート5を設ける前に拡散して
置かねばならず、チャネル形成層6やソース層7のよう
にゲートをマスクとするいわゆる自己整合拡散ができな
いから、フォトプロセスに非常な高精度を要するほか、
工程数が増す問題を持ち込むことになる。
As can be seen from FIG. 3A, the punch-through described above is likely to occur because the electric field is concentrated at the corners of the rectangular diffusion pattern of the channel forming layer 6 and the source layer 7, and this electric field concentration is relaxed as much as possible. Therefore, for example, the connecting layer 6a, which is shown only at one position in the figure, is provided with four adjacent channel forming layers 6.
Conventionally, a device such as an X-shape is provided so that the corners of the are connected to each other. However, since a large amount of channel current originally tends to flow in this corner portion, this means that the current flowing in the corner portion is eliminated, so that the effective peripheral length of the source layer 7 is reduced and the current capacity is considerably reduced. . In addition, the contact layer 6a must be diffused before the gate 5 is provided, and the so-called self-aligned diffusion using the gate as a mask like the channel forming layer 6 and the source layer 7 cannot be performed, which is very important for a photo process. In addition to requiring high precision,
This introduces the problem of increasing the number of processes.

チャネル形成層6およびソース層7を前述のように六
角形に形成するものでは、角の角度が120度になるので
電界集中は方形の90度の場合よりもかなり緩和される
が、実験結果でも上述の連絡層6aを設ける程の効果は得
られない。また、縦形電界効果トランジスタを集積回路
装置に作り込む場合、その微小トランジスタの並列接続
数がふつう数十個程度なので、それらを合理的に六方配
列するのがかなり困難である。すなわち、各微小トラン
ジスタの大きさには利用できるフォトプロセスの精度に
よって下限があるから、予定の面積内に必要個数を納め
ようとすると寸法が半端になって面積の利用効率が落ち
たり、やむなく予定面積を広げなければならなくなって
しまう。
In the case where the channel forming layer 6 and the source layer 7 are formed in a hexagonal shape as described above, since the angle of the corner is 120 degrees, the electric field concentration is considerably relaxed as compared with the case of a square shape of 90 degrees. It is not possible to obtain the effect of providing the above-mentioned connecting layer 6a. Further, when the vertical field effect transistor is built in an integrated circuit device, it is quite difficult to reasonably arrange them in a hexagonal array because the number of parallel connections of the small transistors is usually about several tens. In other words, the size of each small transistor has a lower limit depending on the accuracy of the photo process that can be used, so if you try to fit the required number in the planned area, the size will be cut off and the utilization efficiency of the area will decrease, or the plan will be forced. You have to expand the area.

本発明は従来技術がもつかかる問題を解決し、チャネ
ル部内に電界集中がほとんどなく、大きな電流容量をと
ることができる縦形電界効果トランジスタを得ることを
目的とする。
SUMMARY OF THE INVENTION It is an object of the present invention to solve the problems of the prior art and to obtain a vertical field effect transistor which has almost no electric field concentration in the channel portion and can have a large current capacity.

〔課題を解決するための手段〕 電界効果トランジスタを作り込むべき一方の導電形を
もつ半導体領域の一方の表面をゲート酸化膜を介して覆
うように設けられ半導体領域の一方の表面に通じる細長
でその端が丸みを有する窓が複数個開けられたゲートを
備え、これら複数のゲートの窓それぞれに、窓から周縁
部分をゲート下に入り込ませて他方の導電形で拡散され
たチャネル形成層と、ゲートの窓からチャネル形成層に
達するように一方の導電形で拡散されたソース層と、ソ
ース層内にゲートの細長な窓が延びる方向に複数個配置
され、ソース層を細長な窓が延びる方向に分断すること
なくソース層の表面からチャネル形成層に達するように
他方の導電形で拡散されたコンタクト層とを備え、ゲー
トの窓内のコンタクト層およびソース層の少なくともコ
ンタクト層相互間部分および複数の窓相互間を導電接触
して両層の表面を短絡するようなソース電極を備え、半
導体領域の他方の面側から導出されたドレイン電極を備
えてなることによって達成される。
[Means for Solving the Problems] A long and narrow strip which is provided so as to cover one surface of a semiconductor region having one conductivity type in which a field effect transistor is to be formed through a gate oxide film and communicates with one surface of the semiconductor region. The gate is provided with a plurality of windows having rounded ends, and a channel forming layer diffused in the other conductivity type is formed in each of the windows of the plurality of gates by allowing the peripheral portion of the windows to enter under the gate, A source layer diffused in one conductivity type from the window of the gate to reach the channel forming layer, and a plurality of elongated windows of the gate are arranged in the source layer in a direction in which the elongated window extends, and the source layer extends in the direction in which the elongated window extends. A contact layer diffused in the other conductivity type so as to reach the channel forming layer from the surface of the source layer without dividing the contact layer in the window of the gate and the source layer. At least, it is provided with a source electrode that electrically contacts between the contact layers and between the windows to short-circuit the surfaces of both layers, and a drain electrode derived from the other surface side of the semiconductor region. Achieved by

上記構成において、チャネル形成層およびソース層は
それぞれゲートをマスクとしてその窓から従来と同様に
自己整合的に拡散されるので、いずれも窓の形状に応じ
た細長なパターンに形成される。縦形電界効果トランジ
スタに持たせるべき電流容量は、ソース層1個の細長な
パターンの長さすなわちその周辺長によっても変わる
が、主には従来と同様にチャネル形成層の個数によって
決まり、従って本発明においてもソース層はふつう複数
個ないし多数個がその細長なパターンの側方に並べて並
設される。
In the above structure, since the channel forming layer and the source layer are diffused in a self-aligned manner from the window using the gate as a mask as in the conventional case, both are formed in an elongated pattern according to the shape of the window. The current capacity to be given to the vertical field effect transistor varies depending on the length of the elongated pattern of one source layer, that is, the peripheral length thereof, but is mainly determined by the number of channel forming layers as in the conventional case, and therefore the present invention. Also in this case, a plurality of source layers or a plurality of source layers are usually arranged side by side on the side of the elongated pattern.

さて、縦形電界効果トランジスタ用に割り当てられた
ある一定の面積から最大の電流容量を得るには、各ソー
ス層の細長なパターンの幅ないしゲートに明ける窓のパ
ターンの幅をフォトプロセスの精度上許される限り小さ
くして、できるだけ多数個のソース層をこの面積内に作
り込む必要がある。しかし、上記の構成にいうように、
ソース電極がゲートの窓内でソース層およびコンタクト
層に導電接触され、フォトプロセス上はこのソース電極
またはコンタクト層の幅が最小寸法になる。このため、
本発明においては、このソース電極またはコンタクト層
の幅をフォトプロセス精度から許される最小寸法に選定
するのが、最大の電流容量を得る上で最も望ましいこと
になる。
By the way, in order to obtain the maximum current capacity from a certain area allocated for the vertical field effect transistor, the width of the elongated pattern of each source layer or the width of the window pattern opened in the gate is allowed for the accuracy of the photo process. It is necessary to make it as small as possible and make as many source layers as possible within this area. However, as mentioned in the above configuration,
The source electrode is conductively contacted with the source layer and the contact layer in the window of the gate, and the width of the source electrode or the contact layer is a minimum dimension in photoprocessing. For this reason,
In the present invention, it is most desirable to select the width of the source electrode or the contact layer to the minimum dimension allowed from the photo process accuracy in order to obtain the maximum current capacity.

〔作用〕[Action]

本発明では前述の構成にいうように、ゲートには細長
な窓が明けられ、ゲートをマスクする拡散によりソース
層およびチャネル形成層も細長なストライプ状のパター
ンに形成され、ソース層内にはその細長なパターンに沿
ってコンタクト層が複数個分布配置されるので、従来の
所定方向に並ぶ微小トランジスタを複数個相互にストラ
イプ状にいわば連結した構造になる。従って、従来の各
微小トランジスタごとにあったソース層等の角部が消失
し、チャネル部内に電界集中がほとんどなくなってパン
チスルー電圧が格段に向上される。もちろん、ストライ
プの端には適宜に例えば半円状の丸みをもたせることに
よって、ストライプ状パターンの端部における電界集中
も実用上問題がない程度に緩和でき、場合によっては複
数個のストライプの端同志を連結して端のない1個のル
ープに形成することもできる。
In the present invention, as described above, a narrow window is opened in the gate, and the source layer and the channel formation layer are also formed in a long stripe pattern by diffusion that masks the gate. Since a plurality of contact layers are distributed and arranged along the elongated pattern, it becomes a structure in which a plurality of conventional small transistors arranged in a predetermined direction are connected to each other in a stripe shape. Therefore, the corners of the source layer and the like that exist in each of the conventional microtransistors disappear, the concentration of the electric field in the channel is almost eliminated, and the punchthrough voltage is significantly improved. Of course, by appropriately rounding the edges of the stripes, for example, in the shape of a semi-circle, the electric field concentration at the edges of the stripe pattern can be relaxed to the extent that there is no practical problem. Can also be connected to form a single loop with no ends.

一方、上述のように微小トランジスタが相互連結され
るので、連結されたソース層部分の周辺長が利用できな
いことになるが、実施例で述べるように各ストライプの
幅を狭めて単位面積あたりこれを多数個並べることによ
り、全体としてはソース層の周辺長を従来よりも長くと
って電流容量をむしろ増加させることができる。また、
集積回路装置に作り込む縦形電界効果トランジスタで
は、フォトプロセス精度に制約されることなく与えられ
た面積一杯にストライプないしループの長さを取れるか
ら、面積の利用効率が向上してその結果電流容量が増加
する。
On the other hand, since the minute transistors are interconnected as described above, the peripheral length of the connected source layer portion cannot be used. However, as described in the embodiment, the width of each stripe is narrowed to reduce this per unit area. By arranging a large number of them, it is possible to increase the peripheral length of the source layer as a whole and to increase the current capacity rather than the conventional one. Also,
In a vertical field effect transistor built into an integrated circuit device, the length of a stripe or loop can be taken to fill a given area without being restricted by photo process accuracy, so that the utilization efficiency of the area is improved and the current capacity is consequently increased. To increase.

〔実施例〕〔Example〕

以下、図を参照しながら本発明の実施例を説明する。
第1図は本発明によるnチャネル形の縦形電界効果トラ
ンジスタを集積回路装置内に作り込んだ例を示すもの
で、同図(a)にはその要部拡大平面図が,同図(b)
にはそのX−X矢視断面図が,同図(c)にはそのY−
Y矢視断面図がそれぞれ示されている。この図中の前に
説明した第3図に対応する部分には同じ符号が付されて
いる。
Hereinafter, embodiments of the present invention will be described with reference to the drawings.
FIG. 1 shows an example in which an n-channel vertical field effect transistor according to the present invention is built in an integrated circuit device. FIG. 1 (a) is an enlarged plan view of the main part thereof, and FIG.
The sectional view taken along the line XX is shown in FIG.
A cross-sectional view taken along the arrow Y is shown. In the figure, the same reference numerals are given to the parts corresponding to FIG.

第1図(b)および(c)に示すように、集積回路装
置用の半導体基板1は通例のように例えばp形であっ
て、その表面にいわゆる埋込層として強いn形のドレイ
ン層2がまず拡散され、その上に半導体領域3として通
常のようにエピタキシャル層が例えば10〜20μmの厚み
にn形で成長される。このエピタキシャル層は、その表
面から強いp形の接合分離層を図示の範囲を囲むパター
ンで基板1に達するまで深く拡散することによって、図
の半導体領域3に接合分離される。ドレイン層2から外
部にドレイン端子を導出するには、通例のように強いn
形の接合層を半導体領域3の図示しない個所の表面から
埋込層としてのドレイン層2に達するように拡散した上
で、その表面に導電接触する電極膜を設ける。
As shown in FIGS. 1 (b) and 1 (c), a semiconductor substrate 1 for an integrated circuit device is, for example, p-type as usual, and an n-type drain layer 2 strong as a so-called buried layer on the surface thereof. Is first diffused, and an epitaxial layer is conventionally grown as the semiconductor region 3 to have a thickness of, for example, 10 to 20 .mu.m in the n-type. The epitaxial layer is junction-separated into the semiconductor region 3 in the figure by deeply diffusing a strong p-type junction isolation layer from the surface thereof until reaching the substrate 1 in a pattern surrounding the illustrated range. In order to derive the drain terminal from the drain layer 2 to the outside, as usual, a strong n
A junction layer having a shape is diffused so as to reach the drain layer 2 as a buried layer from the surface of a portion (not shown) of the semiconductor region 3, and then an electrode film which is in conductive contact is provided on the surface.

半導体領域3に縦形電界効果トランジスタを作り込む
に当たっては、まずその表面を0.1μm程度の薄いゲー
ト酸化膜4で覆った上で、ゲート5用に例えば多結晶シ
リコン層を0.5〜1μmの厚みに全面成長させ、それを
フォトエッチングすることによって第1図(a)に示す
ように細長な窓5aを明ける。この実施例における窓5aの
大きさは、例えばその図の上下方向の幅が10μm程度,
左右方向の長さが60μm程度とされ、その両端部の形状
は図示のように半円形とされる。なお、この第1図
(a)は図示の都合上、第3図の場合と同様にソース電
極10を取り除いた状態で示されている。
When fabricating a vertical field effect transistor in the semiconductor region 3, first, the surface is covered with a thin gate oxide film 4 of about 0.1 μm, and then, for example, a polycrystalline silicon layer for the gate 5 is entirely formed with a thickness of 0.5 to 1 μm. By growing it and photoetching it, an elongated window 5a is opened as shown in FIG. 1 (a). The size of the window 5a in this embodiment is, for example, about 10 μm in the vertical width in the figure,
The length in the left-right direction is about 60 μm, and the shape of both ends thereof is semicircular as shown. For convenience of illustration, FIG. 1 (a) is shown with the source electrode 10 removed as in the case of FIG.

ついで、p形のチャネル形成層6を、通例のようなゲ
ート5をマスクとする自己整合方式のイオン注入とそれ
に引き続く熱拡散とにより、所定の不純物濃度で例えば
3μm程度の深さに拡散し、同時にその周縁をゲート5
の下に2〜3μm程度入り込ませる。次に、不純物濃度
が1020原子/cm3程度の強いn形のソース層7を、上と同
様にゲート5をマスクとするイオン注入法により、チャ
ネル形成層6に重ねてただしそれよりは浅い例えば1.5
μmの深さに拡散し、この際その周縁をゲート5の下に
若干入り込ませて、ゲート5の下のチャネル形成層6が
例えば1〜1.5μmのチャネル長を持つようにする。以
上によって、チャネル形成層6およびソース層7は、ゲ
ート5の窓5aと同形の細長なストライプ状パターンで拡
散される。
Then, the p-type channel forming layer 6 is diffused to a depth of, for example, about 3 μm at a predetermined impurity concentration by a conventional self-aligned ion implantation using the gate 5 as a mask and subsequent thermal diffusion. Gate 5 at the same time
It is made to enter under 2 to 3 μm. Next, a strong n-type source layer 7 having an impurity concentration of about 10 20 atoms / cm 3 is overlaid on the channel forming layer 6 by the ion implantation method using the gate 5 as a mask as above, but shallower than that. For example 1.5
It is diffused to a depth of .mu.m, and at this time, its peripheral edge is slightly inserted under the gate 5 so that the channel forming layer 6 under the gate 5 has a channel length of, for example, 1 to 1.5 .mu.m. As described above, the channel forming layer 6 and the source layer 7 are diffused in the elongated striped pattern having the same shape as the window 5a of the gate 5.

p形のコンタクト層8は1019原子/cm3程度の高不純物
濃度とされ、この実施例ではそれぞれ5μm角程度の大
きさの方形パターンで、上のように細長なパターンに形
成されたソース層7内に複数個図示のように並べて、そ
れぞれその下側のチャネル形成層に接続する深さに拡散
され、それらの相互間隔は例えば5μm程度とされる。
なお、この実施例では、コンタクト層8がフォトプロセ
ス上の最小寸法となる。
The p-type contact layer 8 is made to have a high impurity concentration of about 10 19 atoms / cm 3, and in this embodiment, each source layer is formed in a rectangular pattern having a size of about 5 μm square and the elongated pattern as described above. A plurality of them are arranged in the inside of 7 as shown in the drawing, and each is diffused to a depth to connect to the channel forming layer thereunder, and their mutual interval is, for example, about 5 μm.
In this embodiment, the contact layer 8 has the minimum dimension in the photo process.

以上で半導体層の拡散が終わり、ついで酸化膜等の絶
縁膜9を1〜2μmの厚みに全面に被着した上で、それ
にゲートの窓5aよりもやや小さいめの同形のパターンで
窓をフォトエッチングで抜き、さらにその上を覆って第
1図(b)および(c)に示すように、ソース電極10用
にアルミ等の金属膜を1μm程度の厚みで真空蒸着ない
しはスパッタする。このソース電極10は、上述の窓内で
ソース層7およびコンタクト層8に導電接触して両層の
表面を短絡し、これによってコンタクト層8に接続され
ているチャネル形成層6はソース層7とほぼ同電位に置
かれる。
After the diffusion of the semiconductor layer is completed, an insulating film 9 such as an oxide film is deposited on the entire surface to a thickness of 1 to 2 μm, and a window having a similar shape slightly smaller than the window 5a of the gate is formed on the window. It is removed by etching, and further covered therewith, a metal film of aluminum or the like for the source electrode 10 is vacuum-deposited or sputtered to a thickness of about 1 μm as shown in FIGS. 1B and 1C. The source electrode 10 is in conductive contact with the source layer 7 and the contact layer 8 in the above-mentioned window to short-circuit the surfaces of both layers, whereby the channel forming layer 6 connected to the contact layer 8 is connected to the source layer 7. They are placed at almost the same potential.

第2図は本発明の異なる実施例を第1図(a)に対応
する平面図で示すものである。この実施例ではゲート5
に明けられる窓5aは第1図の場合と同じく細長である
が、その幅がさらに狭く例えば7μm程度とされる。p
形のチャネル形成層6およびn形のソース層7をゲート
5をマスクとしてストライプ状に拡散する要領は第1図
の場合と同じで、両層のゲート5の下への入り込み量も
同程度とされる。しかしこの実施例では、これらの層の
拡散の次に絶縁膜9が設けられ、それにゲートの窓5aと
同形であるがその幅が例えば3μm程度の狭い窓が抜か
れる。これがこの実施例におけるフォトプロセス上の最
小寸法になる。
FIG. 2 shows a different embodiment of the present invention in a plan view corresponding to FIG. 1 (a). In this embodiment, gate 5
The window 5a which is opened is elongated as in the case of FIG. 1, but its width is narrower, for example, about 7 μm. p
The procedure for diffusing the channel-shaped channel forming layer 6 and the n-type source layer 7 in a stripe shape using the gate 5 as a mask is the same as in the case of FIG. To be done. However, in this embodiment, an insulating film 9 is provided next to the diffusion of these layers, and a window having the same shape as the window 5a of the gate but having a width of, for example, about 3 μm is removed. This is the minimum size in the photo process in this embodiment.

ついで、コンタクト層8がソース層7内に複数個並べ
て第1図の実施例と同様な要領で,ただし絶縁膜9をマ
スクの一部として拡散される。各コンタクト層8の図の
左右方向の長さは前と同じく例えば5μm程度とされる
が、その図の上下方向の幅は絶縁膜9の窓の幅と同じ3
μmから5μm程度までとなる。この第2図には図示さ
れていないが、ソース電極10は絶縁膜9の窓内でコンタ
クト層8とソース層7のコンタクト層相互間部分に導電
接触するように設けられる。
Then, a plurality of contact layers 8 are arranged in the source layer 7 and diffused in the same manner as in the embodiment of FIG. 1, except that the insulating film 9 is used as a part of the mask. The length of each contact layer 8 in the left-right direction in the figure is, for example, about 5 μm as before, but the width in the up-down direction in the figure is the same as the window width of the insulating film 9.
It is about 5 μm to 5 μm. Although not shown in FIG. 2, the source electrode 10 is provided in the window of the insulating film 9 so as to be in conductive contact with a portion between the contact layers of the contact layer 8 and the source layer 7.

この実施例では、ソース電極10が絶縁膜9の窓内の半
導体層に導電接触する幅をフォトプロセス上許容される
最小寸法,この例では3μmとすることにより、ソース
層7のストライプの幅を狭くして単位面積あたり作り込
むストライプ数を増し、電流容量を第1図の実施例の場
合よりもさらに20%程度増加させることができる。ま
た、この実施例の場合、ソース電極のソース層7および
コンタクト層8との導電接触面積が前の実施例の場合よ
りも減少するが、両層7および8をほぼ同電位に保つこ
とができる。
In this embodiment, the width of the source electrode 10 in conductive contact with the semiconductor layer in the window of the insulating film 9 is set to the minimum dimension allowed in the photo process, which is 3 μm in this example, so that the width of the stripe of the source layer 7 is reduced. By narrowing the number of stripes formed per unit area, the current capacity can be further increased by about 20% compared with the case of the embodiment of FIG. Further, in this embodiment, the conductive contact area of the source electrode with the source layer 7 and the contact layer 8 is smaller than that in the previous embodiment, but both layers 7 and 8 can be maintained at substantially the same potential. .

より高い精度のフォトプロセスを利用できる場合、こ
の最小寸法をさらに小さく取って電流容量を高めること
ができるが、ソース層7のストライプの端部の半径が小
さくなって電界集中の問題が若干出てくるので、第2図
に鎖線Cで示すようにストライプの端を相互に連結し、
全体では例えば前述のようにループ状として、ストライ
プ端での電界集中のおそれをなくすことができる。
If a photo process with higher accuracy can be used, this minimum size can be made smaller to increase the current capacity, but the radius of the end portion of the stripe of the source layer 7 becomes small, and the problem of electric field concentration appears a little. As shown by the chain line C in FIG. 2, connect the ends of the stripes to each other.
As a whole, for example, the loop shape as described above can eliminate the possibility of electric field concentration at the stripe edge.

以上のように構成された本発明による縦形電界効果ト
ランジスタは例えば150〜200Vの回路電圧で使用可能な
耐圧値とチップ面積100平方μmあたり50mA以上の電流
容量を持ち、1ないし4MHzまでの高周波の用途に用いる
ことができる。また、ゲートしきい値については、2V程
度の低い値を安定して保証することができる。
The vertical field effect transistor according to the present invention configured as described above has a withstand voltage value which can be used at a circuit voltage of 150 to 200 V and a current capacity of 50 mA or more per 100 square μm of the chip area, and a high frequency of 1 to 4 MHz. It can be used for various purposes. Further, as for the gate threshold value, a low value of about 2 V can be stably guaranteed.

なお、以上説明した実施例はあくまで例示であり、本
発明はその要旨内で種々の態様で実施をすることができ
る。
The embodiments described above are merely examples, and the present invention can be carried out in various modes within the scope thereof.

〔発明の効果〕〔The invention's effect〕

以上の記載のとおり本発明では、縦形電界効果トラン
ジスタのゲートに明ける窓を細長な形状とし、このゲー
トの窓から従来と同様にチャネル形成層とその内側のソ
ース層とを順次それらの周縁部分をゲート下に入り込ま
せて拡散して両層を二重構造のストライプ状のパターン
に形成し、ストライプ状のソース層内にコンタクト層を
複数個分布配置して拡散した上で、ソース電極をゲート
の窓内のソース層およびコンタクト層に導電接触するよ
うに設けたので、チャネル部を従来の方形ないし六角形
の微小トランジスタを集積化した構造のように電界集中
が起こりやすい角部が全くない形状に形成でき、パンチ
スルー電圧を格段に向上して縦形電界効果トランジスタ
の使用電圧を従来の100V級から200V級にまで上げるとと
もに、ストライプ状のパターンの幅を狭くして単位面積
あたりのストライプ数を増すことによりソース層の周辺
長を増加させて、フォトプロセスの精度によって若干異
なるがトランジスタの電流容量を従来より20〜30%程度
向上することができる。
As described above, in the present invention, the window opened in the gate of the vertical field effect transistor has an elongated shape, and the channel forming layer and the source layer inside the channel forming layer are sequentially formed from the window of the gate in the peripheral portion thereof. Under the gate, diffuse to form both layers in a stripe-shaped pattern with a double structure.Distribute and distribute a plurality of contact layers in the stripe-shaped source layer, and then set the source electrode to the gate. Since it is provided so as to make conductive contact with the source layer and contact layer in the window, the channel has a shape with no corners where electric field concentration is likely to occur, as in the structure in which conventional rectangular or hexagonal microtransistors are integrated. It can be formed, the punch-through voltage is significantly improved, and the operating voltage of the vertical field effect transistor is increased from the conventional 100V class to 200V class, and the stripe-shaped To increase the peripheral length of the source layer by narrowing the turn width and increasing the number of stripes per unit area, and improving the current capacity of the transistor by about 20 to 30% compared to the past, although it may vary slightly depending on the accuracy of the photo process. You can

また、フォトプロセス上の最小寸法を絶縁膜の窓明け
に用いる第2図の実施例に述べた態様によれば、コンタ
クト層を含めて各半導体層の拡散のためのフォトプロセ
スに高精度を要せず、かつフォトプロセス上許される最
小寸法を最大限利用して縦形電界効果トランジスタに大
きな電流容量を持たせることができる。
Further, according to the aspect described in the embodiment of FIG. 2 in which the minimum dimension on the photo process is used for opening the window of the insulating film, the photo process for diffusion of each semiconductor layer including the contact layer requires high accuracy. The vertical field-effect transistor can have a large current capacity without making use of the minimum dimension allowed in the photo process.

以上の特長をもつ本発明は、集積回路装置内に比較的
小型の縦形電界効果トランジスタを複数個組み込む場合
に最適である。すなわち、かかる場合には各トランジス
タに割り当てうる面積には常に制約があるが、本発明に
よる縦形電界効果トランジスタはそのストライプ長を任
意に設定できるので、割当面積を最も有効に利用して面
積あたりの電流容量を大きくとることができる。
The present invention having the above characteristics is most suitable for incorporating a plurality of relatively small vertical field effect transistors in an integrated circuit device. That is, in such a case, there is always a restriction on the area that can be allocated to each transistor, but since the vertical field effect transistor according to the present invention can arbitrarily set its stripe length, the allocated area is used most effectively to A large current capacity can be taken.

【図面の簡単な説明】 第1図および第2図が本発明に関し、第1図は本発明に
よる縦形電界効果トランジスタの実施例の要部拡大平面
図および断面図、第2図は本発明の異なる実施例の要部
拡大平面図である。第3図は従来技術による縦形電界効
果トランジスタの要部拡大平面図である。図において、 1:集積回路装置用半導体基板、2:ドレイン層、3:半導体
領域ないしはエピタキシャル層、4:ゲート酸化膜、5:ゲ
ート、5a,5b:ゲートの窓、6:チャネル形成層、6a:連結
層、7:ソース層、8:コンタクト層、9:絶縁膜、10:ソー
ス電極、11:ドレイン電極、C:ストライプの連結路、D:
ドレイン端子、e:電子、G:ゲート端子、S:ソース端子、
である。
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 and FIG. 2 relate to the present invention. FIG. 1 is an enlarged plan view and a sectional view of an essential part of an embodiment of a vertical field effect transistor according to the present invention, and FIG. It is a principal part enlarged plan view of a different Example. FIG. 3 is an enlarged plan view of a main part of a vertical field effect transistor according to the prior art. In the figure, 1: semiconductor substrate for integrated circuit device, 2: drain layer, 3: semiconductor region or epitaxial layer, 4: gate oxide film, 5: gate, 5a, 5b: window of gate, 6: channel formation layer, 6a : Connecting layer, 7: source layer, 8: contact layer, 9: insulating film, 10: source electrode, 11: drain electrode, C: stripe connecting path, D:
Drain terminal, e: electron, G: gate terminal, S: source terminal,
Is.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】電界効果トランジスタを作り込むべき一方
の導電形をもつ半導体領域の一方の表面をゲート酸化膜
を介して覆うように設けられ半導体領域の一方の表面に
通じる細長でその端が丸みを有する窓が複数個開けられ
たゲートを備え、これら複数のゲートの窓それぞれに、
窓から周縁部分をゲート下に入り込ませて他方の導電形
で拡散されたチャネル形成層と、ゲートの窓からチャネ
ル形成層に達するように一方の導電形で拡散されたソー
ス層と、ソース層内にゲートの細長な窓が延びる方向に
複数個配置され、ソース層を細長な窓が延びる方向に分
断することなくソース層の表面からチャネル形成層に達
するように他方の導電形で拡散されたコンタクト層とを
備え、ゲートの窓内のコンタクト層およびソース層の少
なくともコンタクト層相互間部分および複数の窓相互間
を導電接触して両層の表面を短絡するようなソース電極
を備え、半導体領域の他方の面側から導出されたドレイ
ン電極を備えてなることを特徴とする縦形電界効果トラ
ンジスタ。
1. An elongated semiconductor device which is provided so as to cover one surface of a semiconductor region having one conductivity type in which a field effect transistor is to be formed, with a gate oxide film interposed therebetween, and has a rounded end. Is provided with a gate having a plurality of windows opened, and the windows of the plurality of gates are respectively
In the source layer, a channel forming layer diffused by the other conductivity type by allowing the peripheral portion to enter under the gate from the window, and a source layer diffused by one conductivity type so as to reach the channel forming layer from the window of the gate. A plurality of contacts are arranged in the direction in which the elongated window of the gate extends, and the contacts are diffused by the other conductivity type so as to reach the channel formation layer from the surface of the source layer without dividing the source layer in the direction in which the elongated window extends. A contact layer in the window of the gate and at least a portion between the contact layers of the source layer and a plurality of windows to make a conductive contact to short-circuit the surfaces of both layers. A vertical field-effect transistor comprising a drain electrode led out from the other surface side.
JP63308285A 1988-12-06 1988-12-06 Vertical field effect transistor Expired - Lifetime JPH0834312B2 (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP63308285A JPH0834312B2 (en) 1988-12-06 1988-12-06 Vertical field effect transistor
FR8916139A FR2640081A1 (en) 1988-12-06 1989-12-06 VERTICAL FIELD EFFECT TRANSISTOR
DE3940388A DE3940388A1 (en) 1988-12-06 1989-12-06 DMOS field effect transistor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63308285A JPH0834312B2 (en) 1988-12-06 1988-12-06 Vertical field effect transistor

Publications (2)

Publication Number Publication Date
JPH02154469A JPH02154469A (en) 1990-06-13
JPH0834312B2 true JPH0834312B2 (en) 1996-03-29

Family

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP63308285A Expired - Lifetime JPH0834312B2 (en) 1988-12-06 1988-12-06 Vertical field effect transistor

Country Status (3)

Country Link
JP (1) JPH0834312B2 (en)
DE (1) DE3940388A1 (en)
FR (1) FR2640081A1 (en)

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US5317184A (en) * 1992-11-09 1994-05-31 Harris Corporation Device and method for improving current carrying capability in a semiconductor device
US5798554A (en) * 1995-02-24 1998-08-25 Consorzio Per La Ricerca Sulla Microelettronica Nel Mezzogiorno MOS-technology power device integrated structure and manufacturing process thereof
EP0768714B1 (en) * 1995-10-09 2003-09-17 Consorzio per la Ricerca sulla Microelettronica nel Mezzogiorno - CoRiMMe Construction method for power devices with deep edge ring
EP0772242B1 (en) 1995-10-30 2006-04-05 STMicroelectronics S.r.l. Single feature size MOS technology power device
EP0772241B1 (en) * 1995-10-30 2004-06-09 STMicroelectronics S.r.l. High density MOS technology power device
DE69515876T2 (en) * 1995-11-06 2000-08-17 Consorzio Per La Ricerca Sulla Microelettronica Nel Mezzogiorno, Catania Power device in MOS technology with low output resistance and capacity and its manufacturing process
US6228719B1 (en) 1995-11-06 2001-05-08 Stmicroelectronics S.R.L. MOS technology power device with low output resistance and low capacitance, and related manufacturing process
EP0782201B1 (en) * 1995-12-28 2000-08-30 STMicroelectronics S.r.l. MOS-technology power device integrated structure
EP0841702A1 (en) * 1996-11-11 1998-05-13 STMicroelectronics S.r.l. Lateral or vertical DMOSFET with high breakdown voltage
EP0961325B1 (en) 1998-05-26 2008-05-07 STMicroelectronics S.r.l. High integration density MOS technology power device
SE517852C2 (en) * 1999-12-15 2002-07-23 Ericsson Telefon Ab L M Power transistor module, power amplifier and method of manufacture thereof
JP6858091B2 (en) * 2017-07-18 2021-04-14 株式会社 日立パワーデバイス Semiconductor devices and their manufacturing methods
WO2019077878A1 (en) * 2017-10-17 2019-04-25 富士電機株式会社 Silicon carbide semiconductor device, and manufacturing method of silicon carbide semiconductor device
CN114820498B (en) * 2022-04-20 2025-05-23 上海华力微电子有限公司 Local graph density analysis method of layout

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JPS5688362A (en) * 1979-12-19 1981-07-17 Toshiba Corp Vertical type power mos transistor
JPS5889864A (en) * 1981-11-24 1983-05-28 Hitachi Ltd Insulated gate type semiconductor device
EP0159663A3 (en) * 1984-04-26 1987-09-23 General Electric Company High-density v-groove mos-controlled thyristors, insulated-gate transistors, and mosfets, and methods for fabrication
JPH0614550B2 (en) * 1984-05-26 1994-02-23 株式会社東芝 Semiconductor device
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JPH0821553B2 (en) * 1986-02-03 1996-03-04 株式会社日立製作所 Multiple spreading method
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Also Published As

Publication number Publication date
FR2640081A1 (en) 1990-06-08
DE3940388A1 (en) 1990-08-23
FR2640081B1 (en) 1995-03-17
DE3940388C2 (en) 1993-07-29
JPH02154469A (en) 1990-06-13

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