JPH01191477A - Field-effect transistor - Google Patents
Field-effect transistorInfo
- Publication number
- JPH01191477A JPH01191477A JP63016251A JP1625188A JPH01191477A JP H01191477 A JPH01191477 A JP H01191477A JP 63016251 A JP63016251 A JP 63016251A JP 1625188 A JP1625188 A JP 1625188A JP H01191477 A JPH01191477 A JP H01191477A
- Authority
- JP
- Japan
- Prior art keywords
- semiconductor layer
- layer
- semiconductor
- effect transistor
- 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.)
- Granted
Links
Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/60—Insulated-gate field-effect transistors [IGFET]
- H10D30/64—Double-diffused metal-oxide semiconductor [DMOS] FETs
- H10D30/66—Vertical DMOS [VDMOS] FETs
- H10D30/663—Vertical DMOS [VDMOS] FETs having both source contacts and drain contacts on the same surface, i.e. up-drain VDMOS
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は集積回路装置への組み込み用に適し、比較的電
圧、電流容量が大な電界効果トランジスタないしはMO
S)ランジスタに関する。[Detailed Description of the Invention] [Field of Industrial Application] The present invention is suitable for incorporation into integrated circuit devices, and is suitable for use in field effect transistors or MOs with relatively large voltage and current capacities.
S) Regarding transistors.
上述の集積回路内に組み込まれる電界効果トランジスタ
ないしはMOSトランジスタはディジタル信号の高速処
理用に広く用いられて来たが、最近では集積回路で電圧
、を流容量の大きな負荷を直接駆動できるように、主に
その回路の終段部に100〜200 Vの回路電圧に耐
え数十〜数百mAの電流容量をもつ比較的大容量の電界
効果トランジスタが組み込まれるようになって来た。か
かる用途に適する電界効果トランジスタにはこれまでの
ディジタル信号処理用のトランジスタとは異なる構造が
必要となるが、小形トランジスタと同じプロセスで集積
回路内に作り込め、かつ200〜300−角程度の小面
積内に納まるようにすることが望ましい。いわゆるDM
O3と称される電界効果トランジスタはこの要求を満た
しうるちので、その構造例を第4図および第5図に示す
。第4図はこの種の電界効果トランジスタ1個の断面図
であり、第5図はその上面図である。Field effect transistors or MOS transistors incorporated into the above-mentioned integrated circuits have been widely used for high-speed processing of digital signals, but recently, integrated circuits have been used to directly drive loads with large voltage and current capacity. Relatively large capacity field effect transistors, which can withstand a circuit voltage of 100 to 200 V and have a current capacity of several tens to several hundreds of mA, have come to be incorporated mainly in the final stage of the circuit. Field-effect transistors suitable for such applications require a structure different from conventional transistors for digital signal processing, but they can be fabricated into integrated circuits using the same process as small transistors, and can be made as small as 200 to 300 square meters. It is desirable to fit within the area. So-called DM
A field effect transistor called O3 satisfies this requirement and an example of its structure is shown in FIGS. 4 and 5. FIG. 4 is a sectional view of one field effect transistor of this type, and FIG. 5 is a top view thereof.
第4図において、通常の集積回路装置と同様に例えばp
形の半導体基板21の上面の電界効果トランジスタを作
り込むべき場所に、埋込半導体層22用に強いn形の層
と分離拡散層の埋込半導体層23用に強いp形の層を拡
散しておいた上で、その全面上に比較的高抵抗性のエビ
キシタル層24をn形で所定の厚みに成長させる。この
エビキシタル層24の表面から分離拡散層25を強いp
形で埋込半導体層23に達するまで深く拡散させて、n
形のエビキシタル層24をいずれもp形の半導体基板2
1.埋込半導体I!23および分離拡散層25から接合
分離された半導体領域とする。In FIG. 4, for example, p
A strong n-type layer for the buried semiconductor layer 22 and a strong p-type layer for the buried semiconductor layer 23 of the isolation diffusion layer are diffused in the upper surface of the shaped semiconductor substrate 21 at the location where the field effect transistor is to be fabricated. Then, an n-type evixital layer 24 having a relatively high resistance is grown to a predetermined thickness on the entire surface. A strong p
The n
The evixital layer 24 is formed on a p-type semiconductor substrate 2.
1. Embedded semiconductor I! The semiconductor region is junction-isolated from 23 and the isolation diffusion layer 25.
この半導体領域24内に電界効果トランジスタが作り込
まれるのであるが、その前に表面から強いn形の接続層
26を環状に半導体領域24の下側の埋込半導体Fi2
4に達するように深く拡散する。この接Murlzeか
らは後でドレイン端子りが導出される。A field effect transistor is formed in this semiconductor region 24, but before that, a strong n-type connection layer 26 is formed from the surface in a circular shape to form a buried semiconductor Fi2 under the semiconductor region 24.
Diffuse deeply to reach 4. A drain terminal is later derived from this connection.
次にこの接続層26で囲まれた円形範囲内にp形で第1
の半導体N27を環状に拡散し、その内径部と内孔部と
の表面を図示のように覆うようにゲート28をごく薄い
ゲート絶縁膜28を介して設ける。さらにこのゲートを
マスクとするイオン注入により、n形の第2の半導体層
29を第1の半導体層27の内部に環状に拡散する。Next, in the circular area surrounded by this connection layer 26, a p-type first
The semiconductor N27 is annularly diffused, and a gate 28 is provided via a very thin gate insulating film 28 so as to cover the surfaces of the inner diameter portion and the inner hole portion as shown. Furthermore, by ion implantation using this gate as a mask, the n-type second semiconductor layer 29 is annularly diffused into the first semiconductor layer 27 .
このような半導体層が拡散された半導体基体の表面の絶
縁膜30の窓を介して電極31〜33が設けられる。電
極31は接続層26と導電接触するように環状に設けら
れ、これからドレイン端子りが導出される。電極32は
第1の半導体層27と第2の半導体層29とに共通に導
電接触するように環状に設けられ、これからソース端子
Sが導出される。電極33はゲート28に導電接触する
円状電極で、これからゲート端子Gが導出される。この
ように構成された電界効果トランジスタは第5図かられ
かるようにゲート電極33を中心する同心円状の構造を
有する。Electrodes 31 to 33 are provided through windows in the insulating film 30 on the surface of the semiconductor substrate in which such a semiconductor layer is diffused. The electrode 31 is provided in an annular shape so as to be in conductive contact with the connection layer 26, and a drain terminal is led out from the electrode 31. The electrode 32 is provided in a ring shape so as to be in common conductive contact with the first semiconductor layer 27 and the second semiconductor layer 29, and a source terminal S is led out from the electrode 32. The electrode 33 is a circular electrode in conductive contact with the gate 28, from which a gate terminal G is led out. The field effect transistor constructed in this manner has a concentric structure with the gate electrode 33 at the center, as shown in FIG.
この電界効果トランジスタは例えばドレイン端子りに正
の電圧を掛け、ソース端子Sを接地して用いる。p形の
第1の半導体Ji27のゲート28の下の表面がチャン
ネル形成域であって、従ってこの例での電界効果トラン
ジスタはnチャンネル形である。ゲート端子Gに正の駆
動電圧を与えたとき、ゲート28の下側にチャンネルが
形成されて、n形の第2の半導体層29からこのチャン
ネルを通して半導体領域24に電子がキャリアとして注
入される。This field effect transistor is used, for example, by applying a positive voltage to the drain terminal and by grounding the source terminal S. The surface of the p-type first semiconductor Ji 27 below the gate 28 is a channel formation region, and therefore the field effect transistor in this example is of an n-channel type. When a positive driving voltage is applied to the gate terminal G, a channel is formed under the gate 28, and electrons are injected as carriers from the n-type second semiconductor layer 29 into the semiconductor region 24 through this channel.
図ではこの注入電流がicで示されている。この注入電
流icにより半導体領域に基板が注入されるとその導電
度が増加するので、注入電流icと並列に橋
図で電流ieで示したように電子がソース電番#雀83
2から第1の半導体層27.半導体領域24.埋込半導
体層22および接続1i26を介してドレイン電極31
に流れる。もちろん、この電子電流ieはそれ自体では
持続性はなく、注入電流icが存在することを条件にし
て流れる。In the figure, this injection current is indicated by ic. When the substrate is injected into the semiconductor region by this injection current ic, its conductivity increases.
2 to the first semiconductor layer 27. Semiconductor region 24. Drain electrode 31 via buried semiconductor layer 22 and connection 1i26
flows to Of course, this electron current ie is not sustainable by itself, but flows on the condition that the injection current ic exists.
前述のDMO3構造の電界効果トランジスタは、注入電
流icからすればもちろん横形で、電子電流ieからす
れば縦形であって画形を兼ねた動作をするので、通常の
電界効果トランジスタより電流容量を木質的に上げるこ
とができ、またその各半導体層がおおむね環状で鋭角部
に電界集中が発生しないので、その耐圧値を構造全高め
ることができる利点を有するが、電界効果トランジスタ
を高耐圧化して行くと電流容量を大きく取れなくなって
くる問題点がある。この耐圧値は容易にわかるようにn
形の半導体領域24とp形の第1の半導体層27との間
の接合に逆バイアスが掛かることによって得られている
のであるから、耐圧値を高めるにはこの接合から空乏層
が半導体領域24や第1の半導体層27に延びやすいよ
うにそれらの不純物濃度を低めてやる要がある。しかし
、不純物濃度を下げると抵抗値が上がるので、電’t、
i eが流れにくくなってその貢献分が減少してしま
うことになる。The above-mentioned field effect transistor with the DMO3 structure is of course horizontal in terms of the injection current IC, and vertical in terms of the electron current ie, and operates as an image. Furthermore, since each semiconductor layer is generally annular and electric field concentration does not occur at sharp corners, it has the advantage of increasing the breakdown voltage of the entire structure. There is a problem that it becomes impossible to obtain a large current capacity. As can be easily understood, this breakdown voltage value is n
This is achieved by applying a reverse bias to the junction between the p-type semiconductor region 24 and the p-type first semiconductor layer 27. Therefore, in order to increase the withstand voltage value, a depletion layer is formed from this junction to the semiconductor region 24. It is necessary to lower the concentration of these impurities so that they can easily extend to the first semiconductor layer 27. However, when the impurity concentration is lowered, the resistance value increases, so the current
ie becomes difficult to flow and its contribution decreases.
つまり、この種の電界効果トランジスタにおいても高耐
圧化と大電流化とは相反的な関係になり、例えば電界効
果トランジスタの径を200〜300−程度に抑えた条
件で耐圧値を200〜300V以上に上げてやると、数
mA以下の電流しか取れなくなってしまう、もちろん電
界効果トランジスタの径寸法を増やしてやれば電流容量
をほぼそれに比例して上げることは可能なのであるが、
径の二乗に比例して大きな面積を電界効果トランジスタ
の集積回路等への組み込みのために食われてしまうこと
になる。In other words, even in this type of field effect transistor, there is a reciprocal relationship between increasing the withstand voltage and increasing the current.For example, under the condition that the diameter of the field effect transistor is suppressed to about 200 to 300 V, the withstand voltage value is 200 to 300 V or more. If you increase the current capacity to 1, you will only be able to obtain a current of less than a few mA.Of course, if you increase the diameter of the field effect transistor, you can increase the current capacity almost proportionally.
A large area is consumed in proportion to the square of the diameter to incorporate the field effect transistor into an integrated circuit or the like.
本発明はかかる問題点を解決して、DMO3のもつ利点
を保持しながら占有面積を増加させずに高耐圧で大電流
容量の電界効果トランジスタを得ることを目的とする。It is an object of the present invention to solve these problems and obtain a field effect transistor with high breakdown voltage and large current capacity without increasing the occupied area while retaining the advantages of DMO3.
本発明はDMOS構造の電界効果トランジスタに、一方
の導電形の半導体領域内にその表面から環状に拡散され
た他方の導電形の第1の半導体層と、第1の半導体層内
にその表面から同心環状にかつ内外両側に環状の表面を
残すように第1の半導体層と二重に拡散された一方の導
電形の第2の半導体層と、第1の半導体層の内外いずれ
かの側と残された環状の表面にチャネルを誘導可能にそ
の表面上に設けられた環状のゲートとを設けることによ
って上述の目的達成に成功したのであ外もちろん、本発
明による電界効果トランジスタにおいても、従来と同様
に、その第1の半導体層および第2の半導体層からなる
共通に一方の主端子したとしてたとえばソース端子が導
出され、半導体領域か他方の主端子として例えばドレイ
ン端子が導出される。The present invention provides a field effect transistor having a DMOS structure, including a first semiconductor layer of one conductivity type annularly diffused from the surface of the semiconductor region of the other conductivity type, and a first semiconductor layer of the other conductivity type diffused from the surface of the first semiconductor layer into the first semiconductor layer. A second semiconductor layer of one conductivity type that is doubly diffused with the first semiconductor layer so as to leave annular surfaces on both the inner and outer sides of the first semiconductor layer in a concentric ring shape; By providing the remaining annular surface with an annular gate provided on the surface so as to be able to induce a channel, the above object has been successfully achieved.Of course, the field effect transistor according to the present invention also has the same advantages as the conventional one. Similarly, the first semiconductor layer and the second semiconductor layer commonly have one main terminal, for example, a source terminal, and the other main terminal, for example, a drain terminal.
前述の従来のDMO5構造の電界効果トランジスタでは
ゲートが半導体領域の中心に置かれ、ゲートの周囲長で
ほぼ決まるチャンネル幅を余り大きく取れなかった点に
着目して、本発明は上記構成にいうようにゲートを環状
に形成してその周囲長つまりチャンネル幅を従来よりも
大幅に増加させることにより、同じ耐圧値と同じ専用面
積内で電界効果トランジスタの電流容量を1〜2桁向上
させることに成功したものである。In the conventional DMO5 structure field effect transistor described above, the gate is placed at the center of the semiconductor region, and the channel width, which is approximately determined by the perimeter of the gate, cannot be made very large. By forming the gate in an annular shape and greatly increasing its perimeter, or channel width, compared to conventional devices, we succeeded in increasing the current capacity of a field-effect transistor by one to two orders of magnitude within the same breakdown voltage and dedicated area. This is what I did.
ゲートを環状に形成することに伴って、本発明では第1
の半導体層の径が従来構造よりも大きくなり、その半導
体領域と接合に鋭角部が発生しなくなるので高耐圧化上
も有利になり、その分だけ第1の半導体層や不純物濃度
を上げて注入電流に並列な電流の貢献率を上げることが
できる。従って本発明ではチャンネル幅を増加させたこ
とによる注入電流を増加させたことによる注入電流の増
加とこの貢献分の増加とが相持って、電界効果トランジ
スタの電流容量が向上される。ゲートを円環状に形成す
る場合はその中心部に面積上の余裕ができるので、従来
は前の第4図のように半導体領域24の周縁部に配置さ
れていたドレイン用の接続層26を逆に半導体領域内の
この中心部に設けるのが有利である。これにより半導体
領域が持つ面積を有効に利用した素子設計が可能になる
。本発明の他の有利な実施態様については次項に番べる
とおりである
〔実施例〕
以下第1図から第3図を参照しながら本発明の詳細な説
明する。第1図は本発明による電界効果トランジスタの
実施例を断面で示すもので、第2図(alはゲート等を
円環状に形成した実施例の上面図、第2図(blはこれ
を角環状に形成した実施例の上面図である。In accordance with forming the gate in an annular shape, the present invention provides the first
The diameter of the semiconductor layer is larger than that of the conventional structure, and there are no sharp corners in the junction with the semiconductor region, which is advantageous in terms of high breakdown voltage. It is possible to increase the contribution rate of the current parallel to the current. Therefore, in the present invention, the current capacity of the field effect transistor is improved due to the increase in the injection current due to the increase in the channel width and the increase in this contribution. When forming a gate in an annular shape, there is an area margin at the center, so the drain connection layer 26, which was conventionally placed at the periphery of the semiconductor region 24 as shown in FIG. 4, is reversed. This central location within the semiconductor region is advantageous. This enables device design that effectively utilizes the area of the semiconductor region. Other advantageous embodiments of the invention can be found in the following section. [Example] The invention will now be described in detail with reference to FIGS. 1 to 3. FIG. FIG. 1 shows a cross section of an embodiment of a field effect transistor according to the present invention, and FIG. FIG.
第1図において、この実施例でも半導体基板1はp形と
されており、数十Ω0程度の比抵抗のものがふつう用い
られる。これにn形の埋込半導体層2およびp形の埋込
半導体層3を10〜20Ω/口のシート抵抗に拡散した
後、半導体領域4用にn形のエビキシタル層を20〜3
0−の厚みに10Ω(至)前後の比抵抗になる不純物濃
度で成長させる6強いp形の分離拡散層5を深く拡散さ
せて半導体領域4を半導体基体から接合分離した後、こ
の実施例では他方の主端子としてのドレイン端子りを導
出するための接続層6を半導体領域4の中心部の表面か
ら強いn形で埋込半導体層2に達するように深く拡散さ
せる。In FIG. 1, the semiconductor substrate 1 in this embodiment is also of p-type, and one with a specific resistance of about several tens of ohms is usually used. After diffusing an n-type buried semiconductor layer 2 and a p-type buried semiconductor layer 3 to a sheet resistance of 10 to 20 Ω/hole, an n-type evixital layer is formed for the semiconductor region 4 by 20 to 3 Ω.
In this example, after the semiconductor region 4 is junction-separated from the semiconductor substrate by deeply diffusing the 6 strong p-type isolation diffusion layer 5, which is grown with an impurity concentration that gives a specific resistance of around 10 Ω (maximum) to a thickness of 0- A connection layer 6 for leading out the drain terminal as the other main terminal is deeply diffused from the surface of the center of the semiconductor region 4 in a strong n-type state so as to reach the buried semiconductor layer 2.
これで電界効果トランジスタを作り込む準備ができたの
で、次にp形の第1の半導体層7をこの例では2重の環
状に拡散する。200〜300■の耐圧値を得るには、
この第1の半導体層を10tlfn前後の深さに数百Ω
/口程度のシート抵抗で拡散するのがよい。またかかる
高耐圧用電界効果トランジスタでは、二重環状の第1の
半導体層の環の相互間のゲート8の下になるチャンネル
形成部用に第1の半導体N7の一部としてそれに連続す
るp形ではあるがシート抵抗のより低いチャンネル形成
層7aを第1の半導体層の半分程度の深さに拡散して置
くのがよい。この上のゲート8は前述のように環状で、
内外二重環状の第1の半導体層の各チャンネル形成層7
aの表面を0.1−程度の薄いゲート絶縁膜8aを介し
て共通に覆うように、0.5−程度の厚みに例えば多結
晶シリコンを成長させて作り込まれる。n形の第2の半
導体層9は通例のようにこのゲート8をマスクとするイ
オン注入法により拡散され、1〜2−の深さに10Ω/
口以下の低いシート抵抗で図示のように二重に環状にそ
れぞれ第1の半導体層7の内部に作り込まれる。Now that the field effect transistor is ready to be fabricated, the p-type first semiconductor layer 7 is diffused into a double ring shape in this example. To obtain a pressure resistance value of 200 to 300■,
This first semiconductor layer is connected to a depth of about 10 tlfn by several hundred Ω.
It is best to diffuse it with a sheet resistance of about 1/2 inch. In addition, in such a high-voltage field effect transistor, for a channel formation portion below the gate 8 between the rings of the double-ring-shaped first semiconductor layer, a p-type continuous layer is formed as part of the first semiconductor N7. However, it is preferable to diffuse the channel forming layer 7a, which has a lower sheet resistance, to a depth approximately half that of the first semiconductor layer. The upper gate 8 is annular as mentioned above,
Each channel forming layer 7 of the first semiconductor layer having an inner and outer double ring shape
For example, polycrystalline silicon is grown to a thickness of about 0.5 - so as to commonly cover the surfaces of the gate insulating films 8 a with a gate insulating film 8 a that is about 0.1 - thick. The n-type second semiconductor layer 9 is diffused by ion implantation using this gate 8 as a mask as usual, and is diffused to a depth of 1 to 2-10Ω/2.
As shown in the figure, the semiconductor layer 7 is formed in a double ring shape inside the first semiconductor layer 7 with a sheet resistance as low as that of the semiconductor layer 7.
以上で電界効果トランジスタ用の半導体層とゲートの作
り込みが終わったので、ついでその上に被着された絶縁
1f!JIOの窓を介して、接続層6に導電接触する他
方の主端子用のこの例ではドレイン電極11と、第1の
半導体層7および第2の半導体層9に共通に導電接触す
る一方の主端子用のソース電極12と、ゲート8に導電
接触するゲート電極13とを設ける。これらの電極11
〜13からは図示のように他方の主端子としてのドレイ
ン端子り、 −方の主端子としてのソース端子Sおよび
ゲート端子りが導出される。Now that the semiconductor layer and gate for the field effect transistor have been fabricated, the insulation layer 1f is deposited on top of the semiconductor layer and gate. A drain electrode 11 in this example for the other main terminal in conductive contact with the connection layer 6 and one main terminal in common conductive contact with the first semiconductor layer 7 and the second semiconductor layer 9 through the window of the JIO. A source electrode 12 for a terminal and a gate electrode 13 in conductive contact with the gate 8 are provided. These electrodes 11
As shown in the figure, a drain terminal as the other main terminal, a source terminal S and a gate terminal as the negative main terminals are derived from 13.
第2図(alは以上のように構成された本発明による電
界効果トランジスタのゲートや半導体層が円環状に形成
された場合の上面図である。ドレイン端子りは従来とは
逆に半導体領域の中心部から導出される。また、図から
部分領域5によって囲まれた円形の半導体領域の面積が
本発明による電界効果トランジスタでは非常に有効に利
用されていることが残数できよう。第2図(blは分離
拡散層5で囲まれた半導体領域を方形にして、その中に
ゲートや半導体層を角環状に形成した電界効果トランジ
スタの上面図である。この実施例では周環の4個のかど
部での電界集中が同図(+1)の場合よりも多いので耐
圧値の面ではこれよりも多少不利になるが、そのかわり
に同図(alの場合には遊んでいた4隅部の面積がさら
に有効利用されているので、電界効果トランジスタの電
流容量を円環状の場合よりも増すことが可能である。FIG. 2 (Al is a top view of the field effect transistor according to the present invention configured as described above, when the gate and semiconductor layer are formed in an annular shape.Contrary to the conventional case, the drain terminal is located in the semiconductor region. Further, it can be seen from the figure that the area of the circular semiconductor region surrounded by the partial region 5 is utilized very effectively in the field effect transistor according to the present invention. (bl is a top view of a field effect transistor in which a semiconductor region surrounded by an isolation diffusion layer 5 is made into a rectangular shape, and a gate and a semiconductor layer are formed in a rectangular ring shape. Since the electric field concentration at the corners is higher than in the case of the same figure (+1), it is somewhat disadvantageous in terms of withstand voltage, but instead, the concentration of the electric field at the four corners that were idle in the case of Since the area is more effectively utilized, it is possible to increase the current carrying capacity of the field effect transistor compared to the annular case.
以上の第1図および第2図に示された実施例では、半導
体領域が200〜300μ径ないしは角の場合で200
〜300 Vの耐圧値をもつ電界効果トランジスタの電
流容量を従来の2〜3mAから25〜40+sA程度に
増加させることができる。In the embodiments shown in FIG. 1 and FIG.
The current capacity of a field effect transistor having a breakdown voltage value of ~300 V can be increased from the conventional 2-3 mA to about 25-40+sA.
以上の実施例では第1の半導体層と第2の半導体層とが
二重環状に形成されていたが、第3図はこれらが一重の
環状に形成された実施例を示すものである。もちろん、
環の数が172になっただけ電流容量の点では前の実施
例より不利になるが、それに応じて半導体領域の面積を
かなり大幅に縮少できる。この点を除いて他は前の実施
例と同様であるから説明は省略する。In the above embodiments, the first semiconductor layer and the second semiconductor layer were formed in a double ring shape, but FIG. 3 shows an embodiment in which they are formed in a single ring shape. of course,
Although the number of rings is now 172, the current capacity is disadvantageous compared to the previous embodiment, but the area of the semiconductor region can be reduced accordingly. Except for this point, the rest is the same as the previous embodiment, so the explanation will be omitted.
以上挙げた実施例に限らず、本発明は種々の態様で実施
をすることができる0例えばゲート等の環の形状は円環
状や角環状に限らず楕円環状や扁平な環状にして、かか
る変形環状のユニットを複数個半導体領域内に作り込ん
で電流容量の増加を図ることができる。この際、埋込半
導体層からディスク記憶装置を導出するための接続層は
半導体領域の中心部とは限らず、半導体領域の4隅部に
分散して設けたり、細長な形にしたりして半導体領域の
もつ面積を有効に利用することが可能である。また、実
施例における各半導体層の導電形を逆にして電界効果ト
ランジスタをpチャネル形にすることができる。The present invention is not limited to the embodiments listed above, and the present invention can be carried out in various forms.For example, the shape of the ring such as a gate is not limited to a circular ring or a rectangular ring, but can be made into an elliptical ring or a flat ring. A plurality of annular units can be built into the semiconductor region to increase the current capacity. At this time, the connection layer for leading out the disk storage device from the embedded semiconductor layer is not limited to the center of the semiconductor area, but may be distributed at the four corners of the semiconductor area, or may be formed into an elongated shape. It is possible to effectively utilize the area of the region. Furthermore, the conductivity type of each semiconductor layer in the embodiment can be reversed to make the field effect transistor a p-channel type.
以上述べたとおり本発明では、0MO3構造の電界効果
トランジスタに一方の導電形の半導体領域内にその表面
から環状に拡散された他方の導電形の第1の半導体層と
、第1の半導体層内にその表面から同心環状にかつ内外
両側に環状の表面を残すように第1の半導体層と二重に
拡散された一方の導電形の第2の半導体層と、第1の半
導体層の内外いずれかの側と残された環状の表面にチャ
ネルを誘導可能にその表面上に設けられた環状のゲート
とを設け、第1の半導体層および第2の半導体層から共
通に一方の主端子を、半導体領域から他方の主端子をそ
れぞれ導出するようにしたので、従来のものに比べてそ
のゲート幅を大幅に増加させて、従来と同じ寸法ないし
は面積の半導体領域内に作り込まれる高耐圧の電界効果
トランジスタの電流容量を本発明により従来よりも1〜
2桁増加させることができる。これはゲート幅を増した
だけ半導体領域への注入電流が増加するだけでなく、注
入電流に基づく並列電流の貢献比率を前述のように従来
よりも改善できるからである。As described above, in the present invention, a field effect transistor having a 0MO3 structure includes a first semiconductor layer of the other conductivity type which is annularly diffused from the surface of the semiconductor region of one conductivity type, and A second semiconductor layer of one conductivity type is doubly diffused with the first semiconductor layer so as to leave an annular surface on both the inner and outer sides of the first semiconductor layer in a concentric ring shape from the surface thereof, and A ring-shaped gate is provided on the surface of the remaining ring-shaped surface so as to be able to induce a channel, and one main terminal is commonly connected from the first semiconductor layer and the second semiconductor layer. Since the other main terminals are each led out from the semiconductor region, the gate width is significantly increased compared to the conventional one, and the high withstand voltage electric field created within the semiconductor region of the same size or area as the conventional one. According to the present invention, the current capacity of the effect transistor can be increased by 1 to 1 compared to the conventional one.
It can be increased by two orders of magnitude. This is because not only the current injected into the semiconductor region increases as the gate width increases, but also the contribution ratio of the parallel current based on the injection current can be improved compared to the conventional method as described above.
本発明の実施に当たっては、各半導体層の拡散パターン
やゲートの形状を従来と異ならせるだけで、従来と同じ
製作プロセスで電流容量の大きな電界効果トランジスタ
を集積回路装置内に組み込むことができる0本発明は比
較的高電圧かつ大電流の負荷を直接駆動する集積回路、
例えばプラズマ表示パネルの駆動用集積回路装置等に通
用して上の効果を最も有利に発揮することができる。In implementing the present invention, only by changing the diffusion pattern of each semiconductor layer and the shape of the gate from the conventional one, a field effect transistor with a large current capacity can be incorporated into an integrated circuit device using the same manufacturing process as the conventional one. The invention is an integrated circuit that directly drives relatively high voltage and large current loads;
For example, it can be applied to an integrated circuit device for driving a plasma display panel, and the above effects can be most advantageously exhibited.
第1図から第3図までが本発明に関し、第1図は本発明
による電界効果トランジスタの一実施例の断面図、第2
回はその上面図、第3図は本発明の異なる実施例を示す
電界効果トランジスタの断面図である。第4図以降は従
来技術に関し、第4図は従来の0MO3構造の電界効果
トランジスタの断面図、第5図はその上面図である0図
において、
1:半導体基板、2:半導体領域用埋込半導体層、3:
分離拡散層用埋込半導体層、4:半導体領域ないしはエ
ビキシタル層、5分離拡散層、6:接続層、7:第1の
半導体層、7a:チャンネル形成層、8Xゲー)、8a
:ゲート1色縁膜、9:第2の半導体層、10:絶縁膜
、11〜13:電極、21:半導体基板、22.23
:埋込半導体層、24:半導体領域ないしはエビキシ
タル層、25:分離拡散層、26:接続層、27;第1
の半導体層、28:ゲート、28a:ゲート絶縁膜、2
9:第2の半導体層、30:絶縁膜、31〜33:電極
、D:他方の主端子としてのドレイン端子、G:ゲート
端子、ic;注入電流、te;注入電流に対する並列電
流、Sニ一方の主端子としてのソース端子、である。
第1図
(a) (b)
第2図1 to 3 relate to the present invention, in which FIG. 1 is a cross-sectional view of one embodiment of a field effect transistor according to the present invention, and FIG.
3 is a top view thereof, and FIG. 3 is a sectional view of a field effect transistor showing a different embodiment of the present invention. 4 and subsequent figures relate to the prior art. FIG. 4 is a cross-sectional view of a conventional field effect transistor with an MO3 structure, and FIG. 5 is a top view thereof. Semiconductor layer, 3:
Embedded semiconductor layer for isolation diffusion layer, 4: semiconductor region or evixital layer, 5 isolation diffusion layer, 6: connection layer, 7: first semiconductor layer, 7a: channel forming layer, 8X game), 8a
: Gate single-color edge film, 9: Second semiconductor layer, 10: Insulating film, 11 to 13: Electrode, 21: Semiconductor substrate, 22.23
: Buried semiconductor layer, 24: Semiconductor region or evixital layer, 25: Isolation diffusion layer, 26: Connection layer, 27: First
semiconductor layer, 28: gate, 28a: gate insulating film, 2
9: second semiconductor layer, 30: insulating film, 31 to 33: electrode, D: drain terminal as the other main terminal, G: gate terminal, ic: injection current, te: parallel current to injection current, Sni One of the main terminals is the source terminal. Figure 1 (a) (b) Figure 2
Claims (1)
拡散された他方の導電形の第1の半導体層と、第1の半
導体層内にその表面から同心環状にかつ内外両側に環状
の表面を残すように第1の半導体層と二重に拡散された
一方の導電形の第2の半導体層と、第1の半導体層の内
外いずれかの側と残された環状の表面にチャネルを誘導
可能にその表面上に設けられた環状のゲートとを備え、
第1の半導体層および第2の半導体層から共通に一方の
主端子を、半導体領域から他方の主端子をそれぞれ導出
してなる電界効果トランジスタ。 2)特許請求の範囲第1項記載の電界効果トランジスタ
において、電界効果トランジスタが集積回路装置への組
み込み用であり、半導体領域が他方の導電形の半導体基
体から接合分離された部分領域であり、他方の主端子が
この部分領域としての半導体領域の表面から導出される
ことを特徴とする電界効果トランジスタ。 3)特許請求の範囲第1項記載の電界効果トランジスタ
において、半導体領域からの他方の主端子の導出のため
に第1の半導体層の下側に埋め込まれた一方の導電形の
埋込半導体層と半導体領域の表面からのこの埋込半導体
層に通じるように拡散された接続層とが設けれられ、接
続層から他方の主端子を導出するようにしたことを特徴
とする電界効果トランジスタ。 4)特許請求の範囲第1項記載の電界効果トランジスタ
において、他方の主端子が環状の第1の半導体層の内側
から導出されることを特徴とする電界効果トランジスタ
。 5)特許請求の範囲第1項記載の電界効果トランジスタ
において、第1の半導体層と第2の半導体層とからなる
二重環が内外二重に設けられ、両二重環に対して環状の
ゲートが共通に設けられることを特徴とする電界効果ト
ランジスタ。[Scope of Claims] 1) A first semiconductor layer of the other conductivity type diffused into a semiconductor region of one conductivity type in an annular shape from the surface thereof, and a first semiconductor layer of the other conductivity type diffused in a concentric ring shape from the surface into the first semiconductor layer. and a second semiconductor layer of one conductivity type doubly diffused with the first semiconductor layer so as to leave ring-shaped surfaces on both the inner and outer sides, and a second semiconductor layer of one conductivity type left on either the inner or outer side of the first semiconductor layer. an annular gate provided on the annular surface to be able to guide a channel into the annular surface;
A field effect transistor in which one main terminal is commonly led out from a first semiconductor layer and a second semiconductor layer, and the other main terminal is led out from a semiconductor region. 2) In the field effect transistor according to claim 1, the field effect transistor is for incorporation into an integrated circuit device, and the semiconductor region is a partial region junction-separated from a semiconductor substrate of the other conductivity type, A field effect transistor characterized in that the other main terminal is led out from the surface of the semiconductor region as this partial region. 3) In the field effect transistor according to claim 1, a buried semiconductor layer of one conductivity type buried under the first semiconductor layer for leading out the other main terminal from the semiconductor region. and a connection layer diffused so as to communicate with the buried semiconductor layer from the surface of the semiconductor region, and the other main terminal is led out from the connection layer. 4) The field effect transistor according to claim 1, wherein the other main terminal is led out from inside the annular first semiconductor layer. 5) In the field effect transistor according to claim 1, a double ring consisting of a first semiconductor layer and a second semiconductor layer is provided on an inner and outer side, and an annular ring is provided for both double rings. A field effect transistor characterized in that a gate is provided in common.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63016251A JP2679074B2 (en) | 1988-01-27 | 1988-01-27 | Field effect transistor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63016251A JP2679074B2 (en) | 1988-01-27 | 1988-01-27 | Field effect transistor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01191477A true JPH01191477A (en) | 1989-08-01 |
| JP2679074B2 JP2679074B2 (en) | 1997-11-19 |
Family
ID=11911345
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63016251A Expired - Lifetime JP2679074B2 (en) | 1988-01-27 | 1988-01-27 | Field effect transistor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2679074B2 (en) |
Cited By (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH03219676A (en) * | 1990-01-25 | 1991-09-27 | Toshiba Corp | Semiconductor device and its manufacturing method |
| JPH03270273A (en) * | 1990-03-20 | 1991-12-02 | Mitsubishi Electric Corp | Semiconductor device and its manufacture |
| US5192989A (en) * | 1989-11-28 | 1993-03-09 | Nissan Motor Co., Ltd. | Lateral dmos fet device with reduced on resistance |
| US5349223A (en) * | 1993-12-14 | 1994-09-20 | Xerox Corporation | High current high voltage vertical PMOS in ultra high voltage CMOS |
| US5432370A (en) * | 1992-08-17 | 1995-07-11 | Fuji Electric Co., Ltd. | High withstand voltage M I S field effect transistor and semiconductor integrated circuit |
| EP0982777A1 (en) * | 1998-08-25 | 2000-03-01 | International Business Machines Corporation | Wordline driver circuit using ring-shaped devices |
| JP2006339321A (en) * | 2005-06-01 | 2006-12-14 | Hitachi Ltd | High voltage analog switch IC and ultrasonic diagnostic apparatus using the same |
| JP2010254128A (en) * | 2009-04-24 | 2010-11-11 | Denso Corp | In-vehicle power converter |
| JP2015204375A (en) * | 2014-04-14 | 2015-11-16 | 株式会社ジェイテクト | semiconductor device |
| JP2015204374A (en) * | 2014-04-14 | 2015-11-16 | 株式会社ジェイテクト | Semiconductor device |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS57141965A (en) * | 1981-02-26 | 1982-09-02 | Nippon Telegr & Teleph Corp <Ntt> | Insulated gate type field effect transistor |
| JPS57162359A (en) * | 1981-03-30 | 1982-10-06 | Toshiba Corp | Semiconductor device |
| JPS605568A (en) * | 1983-06-23 | 1985-01-12 | Sanken Electric Co Ltd | Vertical insulated gate field effect transistor |
| JPS63202971A (en) * | 1987-02-19 | 1988-08-22 | Toshiba Corp | Semiconductor device |
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1988
- 1988-01-27 JP JP63016251A patent/JP2679074B2/en not_active Expired - Lifetime
Patent Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS57141965A (en) * | 1981-02-26 | 1982-09-02 | Nippon Telegr & Teleph Corp <Ntt> | Insulated gate type field effect transistor |
| JPS57162359A (en) * | 1981-03-30 | 1982-10-06 | Toshiba Corp | Semiconductor device |
| JPS605568A (en) * | 1983-06-23 | 1985-01-12 | Sanken Electric Co Ltd | Vertical insulated gate field effect transistor |
| JPS63202971A (en) * | 1987-02-19 | 1988-08-22 | Toshiba Corp | Semiconductor device |
Cited By (12)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5192989A (en) * | 1989-11-28 | 1993-03-09 | Nissan Motor Co., Ltd. | Lateral dmos fet device with reduced on resistance |
| JPH03219676A (en) * | 1990-01-25 | 1991-09-27 | Toshiba Corp | Semiconductor device and its manufacturing method |
| JPH03270273A (en) * | 1990-03-20 | 1991-12-02 | Mitsubishi Electric Corp | Semiconductor device and its manufacture |
| US5432370A (en) * | 1992-08-17 | 1995-07-11 | Fuji Electric Co., Ltd. | High withstand voltage M I S field effect transistor and semiconductor integrated circuit |
| US5349223A (en) * | 1993-12-14 | 1994-09-20 | Xerox Corporation | High current high voltage vertical PMOS in ultra high voltage CMOS |
| EP0982777A1 (en) * | 1998-08-25 | 2000-03-01 | International Business Machines Corporation | Wordline driver circuit using ring-shaped devices |
| US6236258B1 (en) | 1998-08-25 | 2001-05-22 | International Business Machines Corporation | Wordline driver circuit using ring-shaped devices |
| JP2006339321A (en) * | 2005-06-01 | 2006-12-14 | Hitachi Ltd | High voltage analog switch IC and ultrasonic diagnostic apparatus using the same |
| JP2010254128A (en) * | 2009-04-24 | 2010-11-11 | Denso Corp | In-vehicle power converter |
| US8742708B2 (en) | 2009-04-24 | 2014-06-03 | Denso Corporation | Electric power conversion apparatus for vehicle |
| JP2015204375A (en) * | 2014-04-14 | 2015-11-16 | 株式会社ジェイテクト | semiconductor device |
| JP2015204374A (en) * | 2014-04-14 | 2015-11-16 | 株式会社ジェイテクト | Semiconductor device |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2679074B2 (en) | 1997-11-19 |
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