JPH10290010A - Silicon carbide semiconductor device and method of manufacturing the same - Google Patents

Silicon carbide semiconductor device and method of manufacturing the same

Info

Publication number
JPH10290010A
JPH10290010A JP10031125A JP3112598A JPH10290010A JP H10290010 A JPH10290010 A JP H10290010A JP 10031125 A JP10031125 A JP 10031125A JP 3112598 A JP3112598 A JP 3112598A JP H10290010 A JPH10290010 A JP H10290010A
Authority
JP
Japan
Prior art keywords
semiconductor layer
region
semiconductor
silicon carbide
groove
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
Application number
JP10031125A
Other languages
Japanese (ja)
Other versions
JP3744175B2 (en
Inventor
Yuichi Takeuchi
有一 竹内
Takamasa Suzuki
孝昌 鈴木
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.)
Denso Corp
Toyota Central R&D Labs Inc
Original Assignee
Denso Corp
Toyota Central R&D Labs Inc
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 Denso Corp, Toyota Central R&D Labs Inc filed Critical Denso Corp
Priority to JP03112598A priority Critical patent/JP3744175B2/en
Publication of JPH10290010A publication Critical patent/JPH10290010A/en
Application granted granted Critical
Publication of JP3744175B2 publication Critical patent/JP3744175B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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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
    • H10D30/668—Vertical DMOS [VDMOS] FETs having trench gate electrodes, e.g. UMOS transistors
    • H—ELECTRICITY
    • H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D64/00—Electrodes of devices having potential barriers
    • H10D64/20—Electrodes characterised by their shapes, relative sizes or dispositions 
    • H10D64/27—Electrodes not carrying the current to be rectified, amplified, oscillated or switched, e.g. gates
    • H10D64/311—Gate electrodes for field-effect devices
    • H10D64/411—Gate electrodes for field-effect devices for FETs
    • H10D64/511—Gate electrodes for field-effect devices for FETs for IGFETs
    • H10D64/517—Gate electrodes for field-effect devices for FETs for IGFETs characterised by the conducting layers
    • H10D64/519—Gate electrodes for field-effect devices for FETs for IGFETs characterised by the conducting layers characterised by their top-view geometrical layouts

Landscapes

  • Insulated Gate Type Field-Effect Transistor (AREA)

Abstract

(57)【要約】 【課題】 炭化珪素からなる縦型絶縁ゲート型電解効果
トランジスタにおいて高信頼性のあるゲート絶縁膜を有
するトランジスタ及びその製造方法を提供する。 【解決手段】 半導体基板4のp型炭化珪素半導体層3
内の表層部における所定領域にはn+ 型ソース領域5が
形成されている。p型炭化珪素半導体層3内の表層部に
おける所定領域には低抵抗p型炭化珪素領域6が形成さ
れている。n+ 型ソース領域5の所定領域に溝7が形成
され、この溝7は、n+ 型ソース領域5とp型炭化珪素
半導体層3を貫通しn- 型炭化珪素半導体層2に達して
いる。溝7は半導体基板4の表面に垂直な側面7aおよ
び半導体基板4の表面に平行な底面7bを有する。溝7
の側面7aにより囲まれた六角形状の領域が島状半導体
領域12となる。島状半導体領域12を囲う側面7aに
ゲート絶縁膜を形成することで信頼性の高いゲート絶縁
膜8を得る。
(57) Abstract: Provided is a vertical insulated gate field effect transistor made of silicon carbide, which has a highly reliable gate insulating film and a method for manufacturing the same. SOLUTION: A p-type silicon carbide semiconductor layer 3 of a semiconductor substrate 4
An n + -type source region 5 is formed in a predetermined region in the surface layer portion. A low-resistance p-type silicon carbide region 6 is formed in a predetermined region in a surface portion of p-type silicon carbide semiconductor layer 3. n + -type grooves 7 in a predetermined region of the source region 5 is formed, the groove 7 extends through the n + -type source region 5 and the p-type silicon carbide semiconductor layer 3 n - has reached the -type silicon carbide semiconductor layer 2 . The groove 7 has a side surface 7 a perpendicular to the surface of the semiconductor substrate 4 and a bottom surface 7 b parallel to the surface of the semiconductor substrate 4. Groove 7
The hexagonal region surrounded by the side surface 7a of FIG. A highly reliable gate insulating film 8 is obtained by forming a gate insulating film on the side surface 7a surrounding the island-shaped semiconductor region 12.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は炭化珪素半導体装置、た
とえば、大電力用縦型絶縁ゲート型電界効果トランジス
タに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a silicon carbide semiconductor device, for example, a high power vertical insulated gate field effect transistor.

【0002】[0002]

【従来技術】近年、電力用トランジスタとして炭化珪素
単結晶材料を使用して作製される縦型パワーMOSFE
Tが提案されている。これは基板表面から半導体基板に
溝を形成し、溝側面をチャネル領域とするものである。
電力用トランジスタにおいてはゲート電圧がオフ時のソ
ースとドレイン間のリーク電流が少なく、かつ、オン時
にはソースとドレイン間の抵抗(以下、オン抵抗とい
う)が小さいことが必要であり、このような要求に対し
て、六方晶炭化珪素の電子物性の長所を生かし、高電圧
印加時のリーク電流の低減とオン抵抗の低減が効果的に
図れる電力用トランジスタとして例えば、特開平7−1
31016号公報や特開平7−326755号公報に記
載のものが提案されている。
2. Description of the Related Art In recent years, a vertical power MOSFE manufactured using a silicon carbide single crystal material as a power transistor.
T has been proposed. In this method, a groove is formed in a semiconductor substrate from the substrate surface, and the side surface of the groove is used as a channel region.
In a power transistor, it is necessary that the leak current between the source and the drain when the gate voltage is off is small and the resistance between the source and the drain when the gate voltage is on (hereinafter referred to as on-resistance) is small. On the other hand, as a power transistor that can effectively reduce the leak current and the on-resistance when a high voltage is applied by taking advantage of the electronic properties of hexagonal silicon carbide, see, for example,
Japanese Patent Application Laid-Open No. 31016 and Japanese Patent Application Laid-Open No. 7-326755 have been proposed.

【0003】[0003]

【発明が解決しようとする課題】しかしながら、特開平
7−131016号公報や特開平7−326755号公
報の溝ゲート型パワーMOSFETにおいては、必ずし
もチャネル移動度が向上するとはいえず、依然としてオ
ン抵抗が高いという問題があった。また、ゲート絶縁膜
の寿命においてシリコンMOSFETに比べて短いとい
う問題があった。
However, in the trench gate type power MOSFETs disclosed in JP-A-7-131016 and JP-A-7-326755, the channel mobility is not necessarily improved, and the on-resistance still remains. There was a problem of high. Further, there is a problem that the life of the gate insulating film is shorter than that of the silicon MOSFET.

【0004】そこで、本発明の目的は、炭化珪素からな
る縦型絶縁ゲート型電解効果トランジスタにおいて高信
頼性のあるゲート絶縁膜を有するトランジスタ及びその
製造方法を提供するものであり、さらにはチャネル移動
度を改善しオン抵抗を効果的に低減することのできるト
ランジスタ及びその製造方法を提供するものである。
An object of the present invention is to provide a transistor having a highly reliable gate insulating film in a vertical insulated gate field effect transistor made of silicon carbide and a method of manufacturing the same. An object of the present invention is to provide a transistor capable of improving the degree of resistance and effectively reducing the on-resistance, and a method for manufacturing the same.

【0005】[0005]

【課題を解決するための手段】請求項1あるいは請求項
5に記載の発明は、縦型絶縁ゲート型電界効果トランジ
スタの溝の側面にて囲まれるとともにチャネル部となる
島状の半導体領域を形成し、その島状半導体領域を囲う
溝側面にゲート絶縁膜を形成した炭化珪素半導体装置を
その要旨とする。つまり島状半導体領域はゲート絶縁膜
により囲われることになる。
According to a first aspect of the present invention, there is provided an island-shaped semiconductor region which is surrounded by a side surface of a groove of a vertical insulated gate field effect transistor and serves as a channel portion. The gist is a silicon carbide semiconductor device in which a gate insulating film is formed on a groove side surface surrounding the island-shaped semiconductor region. That is, the island-shaped semiconductor region is surrounded by the gate insulating film.

【0006】請求項2に記載の発明は、請求項1に記載
の発明における島状半導体領域の平面形状を多角形と
し、かつ、その多角形のいずれの内角も180度未満で
あることをその要旨とする。請求項3あるいは請求項6
に記載の発明は、前記多角形の辺、すなわち溝側面が、
略[11−00]方向に平行であり、かつ、ゲート絶縁
膜はウエット雰囲気の熱酸化で形成された絶縁膜である
ことをその要旨とする。
According to a second aspect of the present invention, the planar shape of the island-shaped semiconductor region in the first aspect of the present invention is a polygon, and the interior angles of any of the polygons are less than 180 degrees. Make a summary. Claim 3 or Claim 6
The invention described in the above, the sides of the polygon, that is, the groove side surface,
The gist is that the gate insulating film is substantially parallel to the [11-00] direction and the gate insulating film is an insulating film formed by thermal oxidation in a wet atmosphere.

【0007】請求項4に記載の発明は、請求項3に記載
の発明における多角形が、各内角が略等しい六角形であ
ることをその要旨とする。以下、本願発明者らの実験及
びその結果に基づく考察により本願発明をより詳細に説
明する。まず、信頼性の高いゲート絶縁膜を得るという
課題に対して、カーボン原子を起源とする界面準位密度
を低下させることができれば、高信頼性のあるゲート絶
縁膜が得られ、ゲート絶縁膜の寿命をものばすことがで
きると考えた。
The gist of the invention described in claim 4 is that the polygon in the invention of claim 3 is a hexagon whose interior angles are substantially equal. Hereinafter, the present invention will be described in more detail based on experiments performed by the present inventors and considerations based on the results. First, with respect to the problem of obtaining a highly reliable gate insulating film, if the interface state density derived from carbon atoms can be reduced, a highly reliable gate insulating film can be obtained. We thought that life could be extended.

【0008】本発明者らは、炭化珪素単結晶基板から構
成される縦型絶縁ゲート型電界効果トランジスタの溝側
面の表面形状が三角形、四角形、六角形、円形等のMO
SFETを設計し、その内側に溝を形成したものと、そ
の外側に溝を形成したものを作製、評価した。その結
果、外側に溝を形成したものの方が相対的にゲート絶縁
膜の寿命も大きいことがわかった。
The inventors of the present invention have proposed a vertical insulated gate field effect transistor composed of a silicon carbide single crystal substrate having an MO having a triangular, quadrangular, hexagonal, circular or other surface shape on the groove side surface.
An SFET was designed, and one having a groove formed inside and one having a groove formed outside the SFET were manufactured and evaluated. As a result, it was found that the life of the gate insulating film was relatively longer when the groove was formed outside.

【0009】この理由について図14及び図15を用い
て説明する。図14(a)、図15(a)は炭化珪素か
らなる縦型絶縁ゲート型電界効果パワーMOSFETの
平面図であり、表面にはソース領域が形成され、かつそ
の側面にチャネル領域が形成されるp型炭化珪素半導体
層3(図15では島状半導体領域12)と溝7及びゲー
ト絶縁膜8が図示されている。また、図14(b)、図
15(b)は図14(a)、図15(a)のそれぞれの
一部拡大図である。図14においてはp型炭化珪素半導
体層3に四角い溝7を形成し、図15においては溝7を
形成することで島状半導体領域12を形成している。す
なわち、図14に示すものが内側に溝を形成したものに
該当し、図15に示すものが外側に溝を形成したものに
該当する。
The reason for this will be described with reference to FIGS. FIGS. 14A and 15A are plan views of a vertical insulated gate field effect power MOSFET made of silicon carbide, in which a source region is formed on the surface and a channel region is formed on a side surface thereof. The p-type silicon carbide semiconductor layer 3 (the island-shaped semiconductor region 12 in FIG. 15), the trench 7 and the gate insulating film 8 are illustrated. FIGS. 14B and 15B are partially enlarged views of FIGS. 14A and 15A, respectively. In FIG. 14, a square groove 7 is formed in the p-type silicon carbide semiconductor layer 3, and in FIG. 15, the island-shaped semiconductor region 12 is formed by forming the groove 7. That is, the one shown in FIG. 14 corresponds to one having a groove formed inside, and the one shown in FIG. 15 corresponds to one having a groove formed outside.

【0010】図14(a)の一部拡大図である図14
(b)に示すように内側に溝を形成したものにおいて
は、チャネル面とチャネル面が交差する角部Aの酸化膜
内で、ゲート絶縁膜形成時の熱酸化で発生するカーボン
原子の拡散が抑えられ、カーボン原子の密度が大きい領
域が存在し、チャネル面とチャネル面が交差する角部で
は、カーボン原子を起源とする界面準位密度が極めて大
きくなり、ゆえにゲート絶縁膜の信頼性の低下を引き起
こすものと結論した。
FIG. 14 is a partially enlarged view of FIG.
In the case where a groove is formed inside as shown in (b), the diffusion of carbon atoms generated by thermal oxidation at the time of forming the gate insulating film is reduced in the oxide film at the corner A where the channel surface intersects. There is a region where the density of carbon atoms is high, and the interface state density originating from carbon atoms becomes extremely large at the corner where the channel surface intersects, so the reliability of the gate insulating film is reduced. Concluded that

【0011】一方、図15(a)の一部拡大図である図
15(b)に示すように外側に溝を形成したものにおい
ては、チャネル面とチャネル面が交差する角部の酸化膜
内で、ゲート絶縁膜形成時の熱酸化で発生するカーボン
原子の拡散が抑制されることはなく、カーボン原子の密
度が特に大きい領域も存在しない。そのため、熱酸化で
発生するカーボン原子の集中によるゲート絶縁膜の信頼
性の低下は発生しないものと結論した。
On the other hand, as shown in FIG. 15 (b), which is a partially enlarged view of FIG. 15 (a), in the case where a groove is formed on the outside, the inside of the oxide film at the corner where the channel surface intersects the channel surface. Thus, diffusion of carbon atoms generated by thermal oxidation during formation of the gate insulating film is not suppressed, and there is no region where the density of carbon atoms is particularly large. Therefore, it was concluded that the reliability of the gate insulating film did not decrease due to the concentration of carbon atoms generated by thermal oxidation.

【0012】尚、内側に溝を形成した場合と、外側に溝
を形成した場合とでゲート絶縁膜形成時の熱酸化で発生
するカーボン原子の拡散が異なる理由としては、図14
(b)、図15(b)の矢印にて示す熱酸化の際のカー
ボン原子が拡散していく経路が図14(b)の内側に溝
を形成したものにおいては特にコーナー部にて密にな
り、一方、図15(b)の外側に溝を形成したものにお
いてはその経路が密になることがないためと考えられ
る。すなわち、内側に溝を形成する場合には凹部となる
領域が形成され、熱酸化の際にカーボン原子が容易に拡
散せず、一方、外側に溝を形成する場合には凹部となる
領域が形成されず凸部になっており、熱酸化の際にカー
ボン原子が容易に拡散するといえる。
The reason why the diffusion of carbon atoms generated by thermal oxidation during the formation of the gate insulating film differs between the case where the groove is formed inside and the case where the groove is formed outside is as follows.
14 (b), the path through which carbon atoms diffuse during thermal oxidation indicated by arrows in FIG. 15 (b) is densely formed especially at the corners in the case where a groove is formed inside FIG. 14 (b). On the other hand, in the case where the groove is formed outside of FIG. 15B, it is considered that the path does not become dense. That is, when a groove is formed on the inside, a region serving as a recess is formed, and carbon atoms are not easily diffused during thermal oxidation. On the other hand, when a groove is formed on the outside, a region serving as a recess is formed. However, it can be said that carbon atoms are easily diffused during thermal oxidation.

【0013】以上説明したように、溝を外側に形成する
ことでゲート絶縁膜の信頼性を高めることができる。ま
た、チャネル移動度が依然として低いという課題に対し
て、本発明者らはトランジスタの電気特性に及ぼすトラ
ンジスタ溝側面の表面形状依存性、チャネル面の結晶面
方位依存性、及び、ゲート絶縁膜形成条件依存性につい
て検討、実験した。
As described above, the reliability of the gate insulating film can be improved by forming the groove outside. In addition, for the problem that the channel mobility is still low, the present inventors depend on the surface shape dependence of the side surface of the transistor groove, the crystal plane orientation dependence of the channel surface, and the conditions for forming the gate insulating film on the electrical characteristics of the transistor. The dependence was examined and tested.

【0014】主表面を(0001−)カーボン面とする
縦型絶縁ゲート型電界効果トランジスタのチャネル面の
面方位すなわち溝側面を5度ずつ変化させたMOSFE
Tを作製し、チャネル移動度を評価した。その結果、ゲ
ート絶縁膜がウエット雰囲気の熱酸化で形成されたMO
SFETではチャネル移動度は60度の周期性を示し、
チャネル面の面方位が[11−00]に平行である場合
にチャネル移動度は極大を示した。また、界面準位密度
を見積もったところ、[11−00]に平行である場合
に極小を示した。図16に本発明者らの評価から得られ
た界面準位密度の面方位依存性を示す。ここで、ゲート
絶縁膜がドライ雰囲気の熱酸化で形成されたMOSFE
Tでは、ウエット雰囲気で形成されたMOSFETより
チャネル移動度は低く、界面準位密度も大きく、強い面
方位依存性を示さなかった。
MOSFE having a main surface of a (0001-) carbon surface and a channel direction of a vertical insulated gate field effect transistor, that is, a MOSFE having a groove side surface changed by 5 degrees.
T was fabricated and the channel mobility was evaluated. As a result, the MO in which the gate insulating film is formed by thermal oxidation in a wet atmosphere is formed.
In the SFET, the channel mobility shows a periodicity of 60 degrees,
When the plane orientation of the channel plane was parallel to [11-00], the channel mobility showed a maximum. In addition, when the interface state density was estimated, it was found to be minimal when it was parallel to [11-00]. FIG. 16 shows the plane orientation dependency of the interface state density obtained from the evaluation of the present inventors. Here, a MOSFE in which a gate insulating film is formed by thermal oxidation in a dry atmosphere.
At T, the channel mobility was lower than that of the MOSFET formed in the wet atmosphere, the interface state density was large, and no strong plane orientation dependence was exhibited.

【0015】この結果はチャネル移動度低下の要因の1
つとして六方晶炭化珪素半導体の結晶構造に起因する界
面準位密度が重要であることを示している。本願発明者
らの考察では、炭化珪素半導体にて形成されたMOSF
ETの界面準位密度の起源は、単原子より構成されるシ
リコン半導体の場合とは異なり、チャネル面に存在する
カーボン原子が重要な役割を担っており、シリコン半導
体から形成されたMOSFETよりも一桁以上大きな値
を示す界面準位密度はカーボン原子に起因するものであ
るとの結論に達した。その理由は、六方晶炭化珪素にお
いて(0001)シリコン面に比べ(0001−)カー
ボン面で界面準位密度が大きいこと、さらに実験で得ら
れた図16の界面準位密度の分布が、結晶構造から数学
的に計算される単位面積当たりのカーボン原子密度とよ
い相関があったからである。
This result is one of the causes of the decrease in channel mobility.
First, the interface state density resulting from the crystal structure of the hexagonal silicon carbide semiconductor is important. The present inventors consider that MOSF formed of a silicon carbide semiconductor
The origin of the interface state density of ET is different from the case of a silicon semiconductor composed of a single atom, in which carbon atoms existing on the channel surface play an important role, and are one more than those of a MOSFET formed from a silicon semiconductor. It was concluded that the interface state density, which is greater than an order of magnitude, was attributed to carbon atoms. The reason is that the hexagonal silicon carbide has a higher interface state density on the (0001-) carbon surface than on the (0001) silicon surface, and the distribution of the interface state density in FIG. This is because there was a good correlation with the carbon atom density per unit area calculated mathematically from

【0016】そこで、チャネル面、及びゲート酸化膜内
に存在するカーボン原子の密度を最大限に減少させ、カ
ーボン原子を起源とする界面準位密度を低下させること
で炭化珪素にて形成したMOSFETのチャネル移動度
向上を図ることができると考えた。それには、チャネル
面を[11−00]に平行とし、ゲート絶縁膜をウエッ
ト雰囲気の熱酸化で形成することが有効であると本発明
者らの実験で確認された。また、図15に示す外側に溝
を形成するものにおいても、上述したようにカーボン原
子がゲート絶縁膜中に取り残されて密となる領域が存在
しないため、カーボン原子に起因する界面準位密度を低
下させてチャネル移動度の向上を図ることができると言
える。
Therefore, the density of the carbon atoms existing in the channel surface and the gate oxide film is reduced to the maximum, and the interface state density originating from the carbon atoms is reduced to reduce the density of the MOSFET formed of silicon carbide. We thought that channel mobility could be improved. It has been confirmed by experiments of the present inventors that it is effective to make the channel surface parallel to [11-00] and to form the gate insulating film by thermal oxidation in a wet atmosphere. Also in the case of forming a groove on the outside shown in FIG. 15, since there is no dense region where carbon atoms are left in the gate insulating film as described above, the interface state density caused by carbon atoms is reduced. It can be said that it is possible to improve the channel mobility by lowering it.

【0017】従って、請求項1あるいは請求項5に記載
の発明によれば、縦型絶縁ゲート型電界効果トランジス
タの溝の側面にて囲まれ、かつチャネル部となる島状の
半導体領域を形成し、つまり、外側に溝を形成して島状
半導体領域の溝側面にゲート絶縁膜を形成するようにし
ているため、熱酸化でゲート絶縁膜を形成する際に、内
側に溝を形成する場合に比べ、炭化珪素の酸化で発生し
たカーボン原子を容易に雰囲気中に拡散することがで
き、これによってカーボン原子の不拡散による界面準位
密度の増大が解消され、チャネル移動度の向上とゲート
酸化膜寿命の向上を図ることができる。
Therefore, according to the first or fifth aspect of the present invention, an island-shaped semiconductor region which is surrounded by the side surface of the groove of the vertical insulated gate field effect transistor and serves as a channel portion is formed. In other words, since the groove is formed on the outside and the gate insulating film is formed on the side surface of the groove of the island-shaped semiconductor region, when forming the groove on the inside when forming the gate insulating film by thermal oxidation, In comparison, carbon atoms generated by the oxidation of silicon carbide can be easily diffused into the atmosphere, thereby eliminating an increase in interface state density due to non-diffusion of carbon atoms, improving channel mobility and improving gate oxide film. The life can be improved.

【0018】請求項2に記載の発明によれば、請求項1
に記載の発明の作用に加え、前記島状半導体領域を多角
形としてあるので、容易な平面形状設計が可能となる。
加えて、前記多角形のいずれの内角も180度未満とし
てあるので、カーボン原子の不拡散による界面準位密度
の増大の解消も可能となる。請求項3あるいは請求項6
に記載の発明によれば、前記多角形の辺、すなわち前記
溝側面は略[11−00]方向に平行であるので、炭化
珪素結晶構造に基づくカーボン原子密度が最小となる面
にMOS界面を形成することができ、本発明者らの実験
結果が示すように、効果的に界面準位密度を低下するこ
とができる。
According to the invention of claim 2, according to claim 1,
In addition to the effect of the invention described in (1), since the island-shaped semiconductor region is polygonal, it is possible to easily design a planar shape.
In addition, since the interior angles of any of the polygons are less than 180 degrees, it is possible to eliminate an increase in interface state density due to non-diffusion of carbon atoms. Claim 3 or Claim 6
According to the invention described in (1), since the sides of the polygon, that is, the groove side surfaces are substantially parallel to the [11-00] direction, the MOS interface is formed on the plane where the carbon atom density based on the silicon carbide crystal structure is minimized. As a result, the interface state density can be effectively reduced as shown by the experimental results of the present inventors.

【0019】請求項4に記載の発明によれば、請求項3
に記載の発明の作用に加え、前記側面の平面形状は、各
内角が略等しい六角形としたので、六角形の各辺におい
て内角をなす角度は略120度となる。よって、縦型絶
縁ゲート型電界効果トランジスタのオフ時にソース・ド
レイン間に高電圧が印加された場合に、側面の形状が六
角形の溝にて形成された半導体部で電界集中によるアバ
ランシェブレークダウンは発生しにくい。すなわち、請
求項3に示すように前記多角形の辺を所定の方向に揃え
るためには三角形や菱形もあり得るがこのような形状で
は鋭角になる部分が生じ電界集中によってアバランシェ
ブレークダウンが生じやすいが、六角形では鋭角になる
領域が存在しないためアバランシェブレークダウンが発
生しにくい。従って、ソース・ドレイン間耐圧設計にお
いては、高抵抗半導体層と第2導電型の半導体層の不純
物濃度及びその膜厚で決まる耐圧を考えればよいので、
高耐圧設計が可能となる。
According to the invention described in claim 4, according to claim 3,
In addition to the effect of the invention described in (1), since the planar shape of the side surface is a hexagon having substantially the same interior angle, the angle forming the interior angle on each side of the hexagon is approximately 120 degrees. Therefore, when a high voltage is applied between the source and the drain when the vertical insulated gate field effect transistor is turned off, avalanche breakdown due to electric field concentration occurs in the semiconductor portion formed by the hexagonal groove on the side surface. Less likely to occur. That is, in order to align the sides of the polygon in a predetermined direction as described in claim 3, there may be a triangle or a rhombus, but in such a shape, an acute angle portion is generated, and avalanche breakdown easily occurs due to electric field concentration. However, an avalanche breakdown is unlikely to occur in a hexagon since there is no region where the angle becomes acute. Therefore, in the source-drain breakdown voltage design, the breakdown voltage determined by the impurity concentration and the film thickness of the high-resistance semiconductor layer and the second conductivity type semiconductor layer may be considered.
High breakdown voltage design becomes possible.

【0020】尚、本明細書においては、六方晶系の単結
晶炭化珪素の面および方向軸を表す場合、本来ならば図
面に記載されているように、所要の数字の上にバーを付
した表現をとるべきであるが、表現手段に制約があるた
めに、前記所要の数字の上にバーを付す表現の代わり
に、前記所要数字の後に「−」を付して表現している。
In the present specification, when the plane and the direction axis of the hexagonal single-crystal silicon carbide are expressed, a bar is added to a required numeral as originally described in the drawings. Although the expression should be taken, due to the restriction of the expression means, instead of the expression in which a bar is added above the required number, the required number is represented by adding "-" after the required number.

【0021】[0021]

【発明の実施の形態】以下、この発明の実施の形態を図
面に従って説明する。図1に本実施の形態におけるnチ
ャネルタイプの縦型絶縁ゲート型電界効果トランジスタ
(以下、縦型パワーMOSFETという)を示す。低抵
抗半導体層としてのn+ 型炭化珪素半導体基板1は、六
方晶炭化珪素が用いられている。このn+ 型炭化珪素半
導体基板1上に、高抵抗半導体層としてのn- 型炭化珪
素半導体層2とp型炭化珪素半導体層3が順次積層され
ている。
Embodiments of the present invention will be described below with reference to the drawings. FIG. 1 shows an n-channel type vertical insulated gate field effect transistor (hereinafter referred to as a vertical power MOSFET) in this embodiment. Hexagonal silicon carbide is used for n + -type silicon carbide semiconductor substrate 1 as a low-resistance semiconductor layer. On this n + -type silicon carbide semiconductor substrate 1, an n − -type silicon carbide semiconductor layer 2 and a p-type silicon carbide semiconductor layer 3 as high-resistance semiconductor layers are sequentially laminated.

【0022】このように、n+ 型炭化珪素半導体基板1
とn- 型炭化珪素半導体層2とp型炭化珪素半導体層3
とから単結晶炭化珪素よりなる半導体基板4が構成され
ており、その上面を略(0001−)カーボン面として
いる。p型炭化珪素半導体層3内の表層部における所定
領域には、半導体領域としてのn+ 型ソース領域5が形
成されている。さらに、p型炭化珪素半導体層3内の表
層部における所定領域には低抵抗p型炭化珪素領域6が
形成されている。
Thus, n + type silicon carbide semiconductor substrate 1
And n − -type silicon carbide semiconductor layer 2 and p-type silicon carbide semiconductor layer 3
Thus, a semiconductor substrate 4 made of single-crystal silicon carbide is formed, and its upper surface is substantially a (0001-) carbon surface. An n + -type source region 5 as a semiconductor region is formed in a predetermined region in a surface portion in p-type silicon carbide semiconductor layer 3. Further, a low-resistance p-type silicon carbide region 6 is formed in a predetermined region in a surface layer portion in p-type silicon carbide semiconductor layer 3.

【0023】又、n+ 型ソース領域5の所定領域に溝7
が形成され、この溝7は、n+ 型ソース領域5とp型炭
化珪素半導体層3を貫通しn- 型炭化珪素半導体層2に
達している。溝7は半導体基板4の表面に垂直な側面7
aおよび半導体基板4の表面に平行な底面7bを有す
る。溝7の側面7aにより囲まれた六角形状の領域(図
1では六角形の一部のみ示す)が島状半導体領域12と
なる。つまり、島状半導体領域12はn- 型炭化珪素半
導体層2上に形成されたp型炭化珪素半導体層3とこの
p型炭化珪素半導体層3に形成されたn+ 型ソース領域
5及び低抵抗p型炭化珪素領域6を備え、他の島状半導
体領域12から分離されている複数の領域のことを言
う。又、本実施形態では溝7の側面7aは略[11−0
0]方向に延設されている。さらに、溝7の側面7aの
平面形状は、各内角が略等しい六角形である。つまり、
図2の基板4の平面図において、六角形の6つの辺をS
1、S2、S3、S4、S5、S6で示し、辺S1とS
2となす角度(内角)、辺S2とS3となす角度(内
角)、辺S3とS4となす角度(内角)、辺S4とS5
となす角度(内角)、辺S5とS6となす角度(内
角)、辺S6とS1となす角度(内角)は略120゜と
なっている。このように島状半導体領域12を形成する
ことでその平面形状に凹部となる領域が形成されない。
A groove 7 is formed in a predetermined region of the n + type source region 5.
Is formed, and penetrates n + -type source region 5 and p-type silicon carbide semiconductor layer 3 to reach n − -type silicon carbide semiconductor layer 2. The groove 7 is a side surface 7 perpendicular to the surface of the semiconductor substrate 4.
a and a bottom surface 7 b parallel to the surface of the semiconductor substrate 4. A hexagonal region (only a part of the hexagon is shown in FIG. 1) surrounded by the side surface 7a of the groove 7 becomes the island-shaped semiconductor region 12. That is, the island-shaped semiconductor region 12 includes the p-type silicon carbide semiconductor layer 3 formed on the n − -type silicon carbide semiconductor layer 2, the n + -type source region 5 formed on the p-type silicon carbide semiconductor layer 3, and the low resistance. A plurality of regions including the p-type silicon carbide region 6 and separated from other island-shaped semiconductor regions 12. In the present embodiment, the side surface 7a of the groove 7 is substantially [11-0].
0] direction. Further, the planar shape of the side surface 7a of the groove 7 is a hexagon whose interior angles are substantially equal. That is,
In the plan view of the substrate 4 shown in FIG.
1, S2, S3, S4, S5, S6, and edges S1 and S
2, the angle between the sides S2 and S3 (the interior angle), the angle between the sides S3 and S4 (the interior angle), the sides S4 and S5
(Inner angle), an angle (inner angle) between sides S5 and S6, and an angle (inner angle) between sides S6 and S1 are approximately 120 °. By forming the island-shaped semiconductor region 12 in this manner, a region that becomes a concave portion in the planar shape is not formed.

【0024】さらに、溝7内での側面7aの表面と溝7
の底面7bにはゲート絶縁膜8が形成されている。溝7
内におけるゲート絶縁膜8の内側には、ゲート電極層9
が充填されている。ゲート電極層9は絶縁膜10にて覆
われている。n+ 型ソース領域5の表面およびと低抵抗
p型炭化珪素領域6の表面には第一の電極層としてのソ
ース電極層11が形成されている。n+ 型炭化珪素半導
体基板1の表面(半導体基板4の裏面)には、第2の電
極層としてのドレイン電極層13が形成されている。
Further, the surface of the side surface 7a in the groove 7 and the groove 7
A gate insulating film 8 is formed on the bottom surface 7b of the substrate. Groove 7
Inside the gate insulating film 8, a gate electrode layer 9 is formed.
Is filled. Gate electrode layer 9 is covered with insulating film 10. Source electrode layer 11 as a first electrode layer is formed on the surface of n + -type source region 5 and the surface of low-resistance p-type silicon carbide region 6. On the surface of n + -type silicon carbide semiconductor substrate 1 (the back surface of semiconductor substrate 4), a drain electrode layer 13 as a second electrode layer is formed.

【0025】このように縦型パワーMOSFETは、チ
ャネル形成面が[11−00]方向に平行となってお
り、図2に示すように六角形の島状半導体領域12の外
側に溝が配置されている。次に、縦型パワーMOSFE
Tの製造工程を、図3〜図8を用いて説明する。まず、
図3に示すように、主表面が略(0001−)カーボン
面であるn+ 型炭化珪素半導体基板1を用意し、その表
面にn- 型炭化珪素半導体層2をエピタキシャル成長
し、さらにn- 型炭化珪素半導体層2上にp型炭化珪素
半導体層3をエピタキシャル成長する。このようにし
て、n+ 型炭化珪素半導体基板1とn - 型炭化珪素半導
体層2とp型炭化珪素半導体層3とからなる半導体基板
4が形成される。
As described above, the vertical power MOSFET is
The channel forming surface is parallel to the [11-00] direction.
As shown in FIG. 2, outside the hexagonal island-shaped semiconductor region 12,
A groove is arranged on the side. Next, the vertical power MOSFET
The manufacturing process of T will be described with reference to FIGS. First,
As shown in FIG. 3, the main surface is substantially (0001-) carbon
N which is a surface+Type silicon carbide semiconductor substrate 1 is prepared and its table
N on face-Type silicon carbide semiconductor layer 2 is epitaxially grown
And then n-P-type silicon carbide on p-type silicon carbide semiconductor layer 2
The semiconductor layer 3 is epitaxially grown. Like this
And n+-Type silicon carbide semiconductor substrate 1 and n -Type silicon carbide semiconductor
Semiconductor substrate comprising body layer 2 and p-type silicon carbide semiconductor layer 3
4 are formed.

【0026】次に、図4に示すように、p型炭化珪素半
導体層3の表層部の所定領域に、n + 型ソース領域5を
例えば窒素のイオン注入により形成する。さらに、p型
炭化珪素半導体層3の表層部の別の所定領域に低抵抗p
型炭化珪素領域6を例えばアルミニウムのイオン注入に
より形成する。そして、図5に示すようにドライエッチ
ング法、例えばRIE(Reactive Ionetching)により、
n+ 型ソース領域5及びp型炭化珪素半導体層3をとも
に貫通してn- 型炭化珪素半導体層2に達する溝7を形
成する。この時、溝7の側面7aが[11−00]方向
に平行となるように溝7を形成し、島状半導体領域12
を形成する。それゆえ、図2に示すように縦型パワーM
OSFETの平面図における島状半導体領域12の形状
が主表面において六角形となる。
Next, as shown in FIG.
In a predetermined region of the surface portion of the conductor layer 3, n +Mold source region 5
For example, it is formed by ion implantation of nitrogen. Furthermore, p-type
Low resistance p is applied to another predetermined region of the surface layer portion of silicon carbide semiconductor layer 3.
Type silicon carbide region 6 for ion implantation of aluminum, for example.
Formed. Then, as shown in FIG.
RIE (Reactive Ionetching)
n+Source region 5 and p-type silicon carbide semiconductor layer 3
Through n-Groove 7 reaching type silicon carbide semiconductor layer 2 is formed.
To achieve. At this time, the side surface 7a of the groove 7 is oriented in the [11-00] direction.
The trench 7 is formed so as to be parallel to the island-shaped semiconductor region 12.
To form Therefore, as shown in FIG.
Shape of island semiconductor region 12 in plan view of OSFET
Are hexagonal on the main surface.

【0027】引き続き、図6に示すように、半導体基板
4および溝7の側面7aと溝7の底面7bにゲート絶縁
膜8を形成する。このとき、ゲート絶縁膜8はウエット
雰囲気の熱酸化で形成する。このウエット酸化はパイロ
ジェニック法と呼ばれる方法で行い、成膜条件としては
上記溝7が形成された半導体基板4を熱酸化炉内に配置
し炉内の温度を1100℃まで上昇させ、水素(H2 )
と酸素(O2 )とを4:3の割合で流入し、水素と酸素
とを燃焼させて水蒸気をつくり、水蒸気と酸素と熱酸化
膜を形成した。本実施形態では酸化膜の成長速度を25
nm/hとし、100nmまで成長させた。これに対し
てドライ酸化は酸素のみを供給して酸化膜を形成する方
法である。そして、図7に示すように、溝7内のゲート
絶縁膜8の内側に、ゲート電極層9を充填する。さら
に、図8に示すように、ゲート電極層9の上面に絶縁膜
10を形成する。その後、図1に示すように、絶縁膜1
0上を含むソース領域5と低抵抗p型炭化珪素領域6の
上にソース電極層11を形成する。又、n+ 型炭化珪素
半導体基板1の表面に、ドレイン電極層12を形成し
て、溝ゲート型パワーMOSFETを完成する。
Subsequently, as shown in FIG. 6, a gate insulating film 8 is formed on the side surface 7a of the semiconductor substrate 4 and the groove 7 and the bottom surface 7b of the groove 7. At this time, the gate insulating film 8 is formed by thermal oxidation in a wet atmosphere. This wet oxidation is performed by a method called a pyrogenic method. As a film forming condition, the semiconductor substrate 4 on which the groove 7 is formed is placed in a thermal oxidation furnace, the temperature in the furnace is increased to 1100 ° C., and hydrogen (H 2 )
And oxygen (O 2 ) were introduced at a ratio of 4: 3, and hydrogen and oxygen were burned to produce steam, thereby forming steam, oxygen, and a thermal oxide film. In this embodiment, the growth rate of the oxide film is 25.
nm / h and grown to 100 nm. On the other hand, dry oxidation is a method of forming an oxide film by supplying only oxygen. Then, as shown in FIG. 7, the inside of the gate insulating film 8 in the trench 7 is filled with the gate electrode layer 9. Further, as shown in FIG. 8, an insulating film 10 is formed on the upper surface of the gate electrode layer 9. Thereafter, as shown in FIG.
The source electrode layer 11 is formed on the source region 5 including the upper region 0 and the low-resistance p-type silicon carbide region 6. Further, a drain electrode layer 12 is formed on the surface of n + type silicon carbide semiconductor substrate 1 to complete a trench gate type power MOSFET.

【0028】以上のように、本実施形態においては溝7
の側面7aにより島状半導体領域12が囲まれるよう
に、かつ図2に示すように平面図において島状半導体領
域12に凹部が形成されないような形状とし、溝7の側
面7aにゲート絶縁膜8を形成しているため、信頼性の
高いゲート絶縁膜8を得ることができる。さらに界面準
位密度を低減でき、チャネル移動度を向上させてオン抵
抗を低減させることもできる。
As described above, in this embodiment, the groove 7
The shape is such that the island-shaped semiconductor region 12 is surrounded by the side surface 7a of the trench 7 and that no recess is formed in the island-shaped semiconductor region 12 in the plan view as shown in FIG. Is formed, a highly reliable gate insulating film 8 can be obtained. Further, the interface state density can be reduced, the channel mobility can be improved, and the on-resistance can be reduced.

【0029】また、本実施形態においては縦型MOSF
ETのチャネルを形成する溝7の側面7aを[11−0
0]方向に平行となるように形成し、かつこのような溝
7の側面7aに対してウエット酸化にてゲート絶縁膜8
を形成しているため図16に示すように界面準位を最も
低減させることができ、これによってチャネル移動度を
向上させることができ、オン抵抗を効果的に低減できる
トランジスタを提供できる。
In this embodiment, the vertical MOSF
The side surface 7a of the groove 7 forming the ET channel is set to [11-0].
0] direction, and the gate insulating film 8 is formed on the side surface 7a of the groove 7 by wet oxidation.
16, the interface state can be reduced most as shown in FIG. 16, whereby the channel mobility can be improved, and a transistor which can effectively reduce on-resistance can be provided.

【0030】これまで述べた構成の他にも、例えば、n
+ 型ソース領域5と低抵抗p型炭化珪素領域6に形成さ
れるソース電極は、異なる材料でもよい。又、低抵抗p
型炭化珪素領域6は省略も可能であり、この場合ソース
電極層11はn+ 型ソース領域5とp型炭化珪素半導体
層3に接するように形成される。又、ソース電極層11
は、少なくともn+ 型ソース領域5の表面に形成されて
いればよい。
In addition to the configuration described above, for example, n
The source electrodes formed in + type source region 5 and low resistance p-type silicon carbide region 6 may be made of different materials. Also, low resistance p
Type silicon carbide region 6 can be omitted. In this case, source electrode layer 11 is formed to be in contact with n + type source region 5 and p type silicon carbide semiconductor layer 3. Also, the source electrode layer 11
May be formed at least on the surface of the n + type source region 5.

【0031】さらに、上述した例では、nチャネル縦型
MOSFETに適用した場合について説明したが、図1
においてp型とn型を入れ替えた、pチャネル縦型MO
SFETにおいても、同じ効果が得られる。さらに、図
1では、溝7は基板表面に対し側面7aがほぼ90゜と
なっているが、図9に示すように、溝7の側面7aと基
板表面のなす角度は必ずしも90゜に近くなくてもよ
い。又、溝7は底面を有しないV字型でもよい。さらに
図10に示すように溝7の側面7aは平面でなくてもよ
く、滑らかな曲面でもよい。尚、溝7の側面7aと基板
表面のなす角度は、チャネル移動度が大きくなるように
設計することにより、より良い効果が得られる。
Further, in the above-described example, the case where the present invention is applied to an n-channel vertical MOSFET has been described.
P-channel vertical MO with p-type and n-type interchanged
The same effect can be obtained in the SFET. Further, in FIG. 1, the side surface 7 a of the groove 7 is substantially 90 ° with respect to the substrate surface, but as shown in FIG. 9, the angle between the side surface 7 a of the groove 7 and the substrate surface is not necessarily close to 90 °. You may. The groove 7 may be V-shaped without a bottom surface. Further, as shown in FIG. 10, the side surface 7a of the groove 7 may not be a flat surface, but may be a smooth curved surface. A better effect can be obtained by designing the angle between the side surface 7a of the groove 7 and the substrate surface so as to increase the channel mobility.

【0032】又、図11に示すように、ゲート電極9の
上部が、n+ 型ソース領域5の上方に延びる形状であっ
てもよい。又、本実施例では島状半導体領域12の表面
形状を六角形としたが、図12に示すように滑らかな楕
円形や円形であっても、また、図13に示すように三角
形状であっても、外側に溝を形成するようにすれば、本
発明の効果が期待できる。
As shown in FIG. 11, the upper portion of gate electrode 9 may have a shape extending above n + type source region 5. In the present embodiment, the surface shape of the island-shaped semiconductor region 12 is hexagonal. However, the surface shape may be a smooth ellipse or circle as shown in FIG. 12, or a triangular shape as shown in FIG. Even so, if the grooves are formed on the outside, the effect of the present invention can be expected.

【図面の簡単な説明】[Brief description of the drawings]

【図1】縦型パワーMOSFETの斜視図。FIG. 1 is a perspective view of a vertical power MOSFET.

【図2】基板の平面図。FIG. 2 is a plan view of a substrate.

【図3】縦型パワーMOSFETの製造工程を説明する
断面図。
FIG. 3 is a cross-sectional view illustrating a manufacturing process of the vertical power MOSFET.

【図4】縦型パワーMOSFETの製造工程を説明する
断面図。
FIG. 4 is a cross-sectional view illustrating a manufacturing process of the vertical power MOSFET.

【図5】縦型パワーMOSFETの製造工程を説明する
断面図。
FIG. 5 is a sectional view illustrating a manufacturing process of the vertical power MOSFET.

【図6】縦型パワーMOSFETの製造工程を説明する
断面図。
FIG. 6 is a sectional view illustrating a manufacturing process of the vertical power MOSFET.

【図7】縦型パワーMOSFETの製造工程を説明する
断面図。
FIG. 7 is a sectional view for explaining a manufacturing process of the vertical power MOSFET.

【図8】縦型パワーMOSFETの製造工程を説明する
断面図。
FIG. 8 is a sectional view for explaining a manufacturing process of the vertical power MOSFET.

【図9】応用例の縦型パワーMOSFETの断面図。FIG. 9 is a cross-sectional view of a vertical power MOSFET of an application example.

【図10】応用例の縦型パワーMOSFETの断面構造
模式図。
FIG. 10 is a schematic sectional view of a vertical power MOSFET according to an application example.

【図11】応用例の縦型パワーMOSFETの断面構造
模式図。
FIG. 11 is a schematic cross-sectional view of a vertical power MOSFET of an application example.

【図12】応用例を説明する基板の平面図。FIG. 12 is a plan view of a substrate illustrating an application example.

【図13】応用例を説明する基板の平面図。FIG. 13 is a plan view of a substrate illustrating an application example.

【図14】(a)は従来の半導体装置を説明する平面
図。(b)は(a)の一部拡大図。
FIG. 14A is a plan view illustrating a conventional semiconductor device. (B) is a partially enlarged view of (a).

【図15】(a)は本発明の半導体装置の概念を説明す
る平面図。(b)は(a)の一部拡大図。
FIG. 15A is a plan view illustrating the concept of a semiconductor device of the present invention. (B) is a partially enlarged view of (a).

【図16】六方晶炭化珪素半導体における界面準位密度
の面方位依存性を示す特性図。
FIG. 16 is a characteristic diagram showing plane orientation dependency of interface state density in a hexagonal silicon carbide semiconductor.

【符号の説明】[Explanation of symbols]

1 n+ 型炭化珪素半導体基板 2 n- 型炭化珪素半導体層 3 p型炭化珪素半導体層 4 半導体基板 5 半n+ 型ソース領域 7 溝 7a 側面 7b 底面 8 ゲート絶縁膜 9 ゲート電極層 10 絶縁膜 11 ソース電極層 13 ドレイン電極層Reference Signs List 1 n + -type silicon carbide semiconductor substrate 2 n -- type silicon carbide semiconductor layer 3 p-type silicon carbide semiconductor layer 4 semiconductor substrate 5 half n + -type source region 7 groove 7 a side surface 7 b bottom surface 8 gate insulating film 9 gate electrode layer 10 insulating film 11 source electrode layer 13 drain electrode layer

Claims (6)

【特許請求の範囲】[Claims] 【請求項1】 第1導電型の低抵抗半導体層と第1導電
型の高抵抗半導体層と第2導電型の半導体層とが順次積
層され、単結晶炭化珪素よりなる半導体基板と、 前記半導体層の表層部の所定領域に形成された第1導電
型の半導体領域と、 前記半導体層の主表面から前記半導体領域と前記半導体
層を共に貫通し前記高抵抗半導体層に達して前記半導体
領域及び前記半導体層を露出させる側面と前記高抵抗半
導体層を露出させる底面とを有する溝と、 前記半導体層及び前記半導体領域とを有し、前記溝の側
面に囲まれるように形成された島状半導体領域と、 少なくとも前記島状半導体領域を囲っている前記溝の側
面に形成されたゲート絶縁膜と、 前記ゲート絶縁膜上に形成されたゲート電極層と、 前記主表面のうち少なくとも前記島状半導体領域におけ
る前記半導体領域の表面に形成された第1の電極と、 前記低抵抗半導体層の裏面に形成された第2の電極とを
備えたことを特徴とする炭化珪素半導体装置。
1. A semiconductor substrate made of single-crystal silicon carbide, in which a low-resistance semiconductor layer of a first conductivity type, a high-resistance semiconductor layer of a first conductivity type, and a semiconductor layer of a second conductivity type are sequentially stacked. A first conductivity type semiconductor region formed in a predetermined region of a surface layer portion of the layer; and a semiconductor region extending from a main surface of the semiconductor layer through the semiconductor region and the semiconductor layer to reach the high resistance semiconductor layer. A groove having a side surface exposing the semiconductor layer and a bottom surface exposing the high-resistance semiconductor layer; an island-shaped semiconductor having the semiconductor layer and the semiconductor region and formed to be surrounded by the side surface of the groove A region, a gate insulating film formed on at least a side surface of the trench surrounding the island-shaped semiconductor region, a gate electrode layer formed on the gate insulating film, and at least the island-shaped semiconductor in the main surface Territory A silicon carbide semiconductor device, comprising: a first electrode formed on a surface of the semiconductor region in a region; and a second electrode formed on a back surface of the low-resistance semiconductor layer.
【請求項2】 前記島状半導体領域は、その平面形状が
多角形であり、かつ、前記多角形のいずれの内角も18
0度未満である請求項1に記載の炭化珪素半導体装置。
2. The island-shaped semiconductor region has a polygonal planar shape, and each interior angle of the polygon is 18
The silicon carbide semiconductor device according to claim 1, wherein the angle is less than 0 degrees.
【請求項3】 前記多角形の辺は、略[11−00]に
平行であり、前記ゲート絶縁膜はウエット雰囲気の熱酸
化にて形成された熱酸化膜である請求項2に記載の炭化
珪素半導体装置。
3. The carbonization device according to claim 2, wherein sides of the polygon are substantially parallel to [11-00], and the gate insulating film is a thermal oxide film formed by thermal oxidation in a wet atmosphere. Silicon semiconductor device.
【請求項4】 前記多角形は、各内角が略等しい六角形
である請求項3に記載の炭化珪素半導体装置。
4. The silicon carbide semiconductor device according to claim 3, wherein said polygon is a hexagon whose interior angles are substantially equal.
【請求項5】 第1導電型の低抵抗半導体層と第1導電
型の高抵抗半導体層と第2導電型の半導体層とを順次積
層し、単結晶炭化珪素よりなる半導体基板を用意する第
1工程と、 前記半導体層の表層部の所定領域に第1導電型の半導体
領域を形成する第2工程と、 前記半導体層の主表面から前記半導体領域と前記半導体
層を共に貫通し前記高抵抗半導体層に達して前記半導体
領域及び前記半導体層を露出させる側面と前記高抵抗半
導体層を露出させる底面とを有する溝を形成し、前記半
導体層及び前記半導体領域とを有して前記溝の側面に囲
まれる島状半導体領域を形成する第3工程と、 少なくとも前記島状半導体領域を囲っている前記溝の側
面にゲート絶縁膜を形成する第4工程と、 前記ゲート絶縁膜上にゲート電極層を形成する第5工程
と、 前記主表面のうち少なくとも前記島状半導体領域におけ
る前記半導体領域の表面に第1の電極を形成し、前記低
抵抗半導体層の裏面に第2の電極を形成する第6工程と
を備えたことを特徴とする炭化珪素半導体装置。
5. A semiconductor substrate made of single-crystal silicon carbide by sequentially laminating a first-conductivity-type low-resistance semiconductor layer, a first-conductivity-type high-resistance semiconductor layer, and a second-conductivity-type semiconductor layer. A second step of forming a first conductivity type semiconductor region in a predetermined region of a surface layer portion of the semiconductor layer; and a high resistance which penetrates both the semiconductor region and the semiconductor layer from a main surface of the semiconductor layer. Forming a groove having a side surface reaching the semiconductor layer and exposing the semiconductor region and the semiconductor layer and a bottom surface exposing the high-resistance semiconductor layer; and forming a groove having the semiconductor layer and the semiconductor region and a side surface of the groove. A third step of forming an island-shaped semiconductor region surrounded by; a fourth step of forming a gate insulating film on at least side surfaces of the trench surrounding the island-shaped semiconductor region; and a gate electrode layer on the gate insulating film. Fifth process to form And a sixth step of forming a first electrode on at least the surface of the semiconductor region in the island-shaped semiconductor region of the main surface, and forming a second electrode on the back surface of the low-resistance semiconductor layer. A silicon carbide semiconductor device characterized by the above-mentioned.
【請求項6】 前記第3工程において、前記溝の側面は
略[11−00]方向に平行に形成され、かつ前記第4
工程において、前記ゲート絶縁膜はウエット雰囲気の熱
酸化にて形成されるものである請求項5に記載の炭化珪
素半導体装置。
6. In the third step, the side surface of the groove is formed substantially parallel to the [11-00] direction, and
6. The silicon carbide semiconductor device according to claim 5, wherein in said step, said gate insulating film is formed by thermal oxidation in a wet atmosphere.
JP03112598A 1997-02-14 1998-02-13 Silicon carbide semiconductor device and manufacturing method thereof Expired - Lifetime JP3744175B2 (en)

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JP9-30410 1997-02-14
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Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002083963A (en) * 2000-06-30 2002-03-22 Toshiba Corp Semiconductor element
JP2009231545A (en) * 2008-03-24 2009-10-08 Fuji Electric Device Technology Co Ltd Silicon carbide mos semiconductor device
WO2012120359A3 (en) * 2011-03-09 2012-11-15 Toyota Jidosha Kabushiki Kaisha Insulated-gate bipolar transistor
JP2014123768A (en) * 2008-12-01 2014-07-03 Fuji Electric Co Ltd Silicon carbide semiconductor element manufacturing method and silicon carbide semiconductor element
US11004936B2 (en) 2018-06-01 2021-05-11 Fuji Electric Co., Ltd. Silicon carbide insulated-gate power field effect transistor

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002083963A (en) * 2000-06-30 2002-03-22 Toshiba Corp Semiconductor element
JP2009231545A (en) * 2008-03-24 2009-10-08 Fuji Electric Device Technology Co Ltd Silicon carbide mos semiconductor device
JP2014123768A (en) * 2008-12-01 2014-07-03 Fuji Electric Co Ltd Silicon carbide semiconductor element manufacturing method and silicon carbide semiconductor element
WO2012120359A3 (en) * 2011-03-09 2012-11-15 Toyota Jidosha Kabushiki Kaisha Insulated-gate bipolar transistor
CN103403872A (en) * 2011-03-09 2013-11-20 丰田自动车株式会社 Insulated-gate bipolar transistor
US9425271B2 (en) 2011-03-09 2016-08-23 Toyota Jidosha Kabushiki Kaisha Insulated-gate bipolar transistor
US11004936B2 (en) 2018-06-01 2021-05-11 Fuji Electric Co., Ltd. Silicon carbide insulated-gate power field effect transistor

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