JPH0546705B2 - - Google Patents

Info

Publication number
JPH0546705B2
JPH0546705B2 JP60278367A JP27836785A JPH0546705B2 JP H0546705 B2 JPH0546705 B2 JP H0546705B2 JP 60278367 A JP60278367 A JP 60278367A JP 27836785 A JP27836785 A JP 27836785A JP H0546705 B2 JPH0546705 B2 JP H0546705B2
Authority
JP
Japan
Prior art keywords
drain
region
source
channel region
semiconductor
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
JP60278367A
Other languages
Japanese (ja)
Other versions
JPS62136077A (en
Inventor
Toshio Baba
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.)
NEC Corp
Original Assignee
Nippon 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP27836785A priority Critical patent/JPS62136077A/en
Publication of JPS62136077A publication Critical patent/JPS62136077A/en
Publication of JPH0546705B2 publication Critical patent/JPH0546705B2/ja
Granted legal-status Critical Current

Links

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は半導体装置に関する。[Detailed description of the invention] (Industrial application field) The present invention relates to a semiconductor device.

(従来の技術) 従来の代表的な半導体装置はSiのMOSFET
(Metal Oxide Semiconductor Field Effect
Transistor)とバイポーラ・トランジスタであ
る。そのうち、MOSFETは動作原理、構造およ
び製造プロセスが簡単なため、高集積化に適し広
く用いられている。
(Conventional technology) A typical conventional semiconductor device is a Si MOSFET.
(Metal Oxide Semiconductor Field Effect
Transistor) and bipolar transistor. Among them, MOSFETs are suitable for high integration and are widely used because of their simple operating principle, structure, and manufacturing process.

MOSFETの断面図を第3図に示す。 Figure 3 shows a cross-sectional view of the MOSFET.

第3図において、1はp型半導体基板、2はn
型不純物を有するソース領域、3はソース領域2
とオーミツク接合を形成するソース電極、4はn
型不純物を有するドレイン領域、5はドレイン領
域5とオーミツク接合を形成するドレイン電極、
6はp型半導体基板1上に設けられたゲート絶縁
膜、7はゲート絶縁膜6上に設けられたゲート電
極、8はソース・ドレイン間の半導体基板1表面
に形成されるチヤネルである。
In FIG. 3, 1 is a p-type semiconductor substrate, 2 is an n-type semiconductor substrate, and 2 is an n-type semiconductor substrate.
Source region with type impurity, 3 is source region 2
and the source electrode forming an ohmic junction, 4 is n
a drain region having a type impurity; 5 a drain electrode forming an ohmic contact with the drain region 5;
6 is a gate insulating film provided on the p-type semiconductor substrate 1, 7 is a gate electrode provided on the gate insulating film 6, and 8 is a channel formed on the surface of the semiconductor substrate 1 between the source and drain.

次にこのMOSFETの動作をソース・ドレイン
間のバンド構造を示す図を用いて説明する。
Next, the operation of this MOSFET will be explained using a diagram showing the band structure between the source and drain.

第4図a,bは第3図のソース領域、半導体基
板表面、ドレイン領域にわたる模式的なバンド構
造を示した図であり、第4図aは熱平衡状態にお
けるバンド図、第4図bはゲート電極7に正電圧
を印加しソース・ドレイン間にチヤネル8が形成
された時のバンド図である。尚、第4図a,bに
おいてEcは伝導帯端、Evは充満帯端、Efはフエ
ルミ準位である。
Figures 4a and 4b are diagrams showing schematic band structures spanning the source region, semiconductor substrate surface, and drain region in Figure 3. Figure 4a is a band diagram in a thermal equilibrium state, and Figure 4b is a gate FIG. 7 is a band diagram when a positive voltage is applied to the electrode 7 and a channel 8 is formed between the source and drain. In FIGS. 4a and 4b, Ec is the conduction band edge, Ev is the filling band edge, and Ef is the Fermi level.

第4図aに示すように、ゲート電圧が0Vの場
合(熱平衡状態)にはソース・ドレイン間の半導
体基板表面にはpn接合による障壁が存在するた
め、ソース・ドレイン間に電圧(ドレイン電圧)
を印加しても電子はソース領域2からドレイン領
域4へ移動することはできない。一方、ゲート電
極7に正電圧が印加されると半導体基板表面には
電子が誘起され、チヤネル(反転層)が形成され
て第4図bに示すバンド構造となる。この状態で
は、ソース・ドレイン間の半導体基板表面にはも
はやpn接合による障壁は存在せず、電子は容易
にソース領域2からドレイン領域4へ移動するこ
とができる。このように、MOSFETではソー
ス・ドレイン間の電流(ドレイン電流)をゲート
電圧で制御するのである。
As shown in Figure 4a, when the gate voltage is 0V (thermal equilibrium state), there is a barrier due to a pn junction on the semiconductor substrate surface between the source and drain, so the voltage between the source and drain (drain voltage)
Even if the voltage is applied, electrons cannot move from the source region 2 to the drain region 4. On the other hand, when a positive voltage is applied to the gate electrode 7, electrons are induced on the surface of the semiconductor substrate, forming a channel (inversion layer), resulting in the band structure shown in FIG. 4b. In this state, there is no longer a barrier due to the pn junction on the surface of the semiconductor substrate between the source and drain, and electrons can easily move from the source region 2 to the drain region 4. In this way, in a MOSFET, the current between the source and drain (drain current) is controlled by the gate voltage.

(発明が解決しようとする問題点) 上述した従来のMOSFETにおいては、原理的
に相互コンダクタンス(ゲート電圧の変化に対す
るドレイン電流の変化分)がゲート電圧に単に比
例するため負荷駆動能力が小さく、高集積化に伴
なつて配線容量の増大および外部負荷の駆動によ
る遅延の割合が増大するため、高速動作が抑制さ
れるという問題がある。この問題を解決するに
は、バイポーラ・トランジスタと同様に相互コン
ダクタンスの非線形性を強め負荷駆動能力を高め
ることが必要である。
(Problems to be Solved by the Invention) In the conventional MOSFET described above, in principle, the mutual conductance (change in drain current with respect to change in gate voltage) is simply proportional to gate voltage, so the load driving ability is small and high There is a problem in that high-speed operation is suppressed because the wiring capacitance increases and the delay rate due to driving an external load increases with integration. To solve this problem, it is necessary to strengthen the nonlinearity of the mutual conductance and increase the load driving ability, similar to bipolar transistors.

本発明の目的は、超高速動作が可能な半導体装
置を提供することにある。
An object of the present invention is to provide a semiconductor device capable of ultra-high-speed operation.

(問題点を解決するための手段) 本発明の半導体装置は、半導体又は絶縁物から
なる基板上に形成された一導電型の不純物を高濃
度に含有し縮退状態に近く反転層が形成されない
半導体からなるチヤネル領域と、このチヤネル領
域を挟み前記基板上に形成された逆導電型の高濃
度不純物を有する縮退した半導体からなるソース
領域およびドレイン領域と、チヤネル領域の表面
に設けられたゲート絶縁膜と、該ゲート絶縁膜上
に設けられたゲート電極と、前記ソース領域およ
びドレイン領域とそれぞれオーミツク接触を形成
するソース電極およびドレイン電極とを有して構
成される。
(Means for Solving the Problems) A semiconductor device of the present invention is a semiconductor which is formed on a substrate made of a semiconductor or an insulator and which contains impurities of one conductivity type at a high concentration and is close to a degenerate state and in which no inversion layer is formed. a channel region consisting of a channel region, a source region and a drain region made of a degenerate semiconductor having high concentration impurities of opposite conductivity type formed on the substrate with the channel region sandwiched therebetween, and a gate insulating film provided on the surface of the channel region. , a gate electrode provided on the gate insulating film, and a source electrode and a drain electrode forming ohmic contact with the source region and the drain region, respectively.

(作用) このように構成された本発明の半導体装置にお
いては、ゲート電圧によりソース・チヤネル領域
表面間およびチヤネル領域表面・ドレイン間のキ
ヤリアのトンネル確率を変化させてドレイン電流
を制御する。トンネル確率は電位差およびpn接
合の空乏層厚の指数関数で変化するため、相互コ
ンダクタンスは大きな非線形性を有する。
(Function) In the semiconductor device of the present invention configured as described above, the drain current is controlled by changing the tunneling probability of carriers between the source and the channel region surface and between the channel region surface and the drain using the gate voltage. Since the tunneling probability changes as an exponential function of the potential difference and the pn junction depletion layer thickness, the mutual conductance has large nonlinearity.

(実施例) 次に、本発明の実施例について図面を参照して
説明する。
(Example) Next, an example of the present invention will be described with reference to the drawings.

第1図は本発明の一実施例の断面図である。 FIG. 1 is a sectional view of an embodiment of the present invention.

第1図において、9は高濃度のp型不純物を含
有しているが縮退するには到つていない半導体層
からなるチヤネル領域である。この実施例の各層
は、p型半導体基板1としてアクセプタ濃度が5
×1018cm-3程度のSi、n型ソース領域2およびド
レイン領域4としてドナー濃度が5×1019cm-3
度のSi、ソース電極3およびドレイン電極5とし
てAl、ゲート絶縁膜6として厚さ100Å程度の熱
酸化SiO2、ゲート電極7としてp型のポリシリ
コン、p型チヤネル領域9として厚さ200Å程度
でアクセプタ濃度が1×1019cm-3程度のSiを用い
た。また、ソース・ドレイン間は500Å程度であ
る。
In FIG. 1, reference numeral 9 denotes a channel region made of a semiconductor layer that contains a high concentration of p-type impurity but has not reached degeneracy. Each layer in this example has an acceptor concentration of 5 as the p-type semiconductor substrate 1.
Si with a donor concentration of approximately ×10 18 cm -3 as the n-type source region 2 and drain region 4, Al with a donor concentration of approximately 5 × 10 19 cm -3 as the source electrode 3 and drain electrode 5, and a thickness as the gate insulating film 6. Thermal oxidation SiO 2 with a thickness of about 100 Å, p-type polysilicon as the gate electrode 7, and Si with a thickness of about 200 Å and an acceptor concentration of about 1×10 19 cm -3 as the p-type channel region 9 were used. Further, the distance between the source and drain is about 500 Å.

次にこの実施例の動作をバンド構造を示す第2
図を用いて説明する。
Next, the operation of this example will be explained in the second section showing the band structure.
This will be explained using figures.

第2図a,bは第1図のソース領域2からチヤ
ネル領域9の表面を経てドレイン領域4にわたる
模式的なバンド構造を示した図であり、第2図a
は熱平衡状態のバンド図、第2図bはゲート電極
に負電圧を印加しチヤネル領域表面に縮退した蓄
積層を形成したときのバンド図である。
2a and 2b are diagrams showing a schematic band structure extending from the source region 2 in FIG. 1 through the surface of the channel region 9 to the drain region 4, and FIG.
is a band diagram in a thermal equilibrium state, and FIG. 2b is a band diagram when a negative voltage is applied to the gate electrode to form a degenerate accumulation layer on the surface of the channel region.

第2図aに示す熱平衡状態では、n型ソース領
域およびドレイン領域のSiとp型チヤネル領域の
Siとの間にはpn接合による電子の障壁が形成さ
れている。チヤネル領域のアクセプタ濃度は縮退
を起こすほどは高くないためこの障壁の幅は100
Å以上と広く、この障壁をトンネル効果で抜ける
確率はほとんどない。したがつて、ソース・ドレ
イン間に0.1V程度の微小電圧を印加してもドレ
イン電流はほとんど流れない。
In the thermal equilibrium state shown in Figure 2a, Si in the n-type source and drain regions and Si in the p-type channel region are
An electron barrier is formed between it and Si by a pn junction. Since the acceptor concentration in the channel region is not high enough to cause degeneracy, the width of this barrier is 100
The barrier is wide, more than Å, and there is almost no probability of tunneling through this barrier. Therefore, even if a minute voltage of about 0.1V is applied between the source and drain, almost no drain current flows.

一方、第2図bに示すようにゲート電極7に負
電圧を印加してチヤネル領域表面に正孔の蓄積層
を形成すると、このチヤネル領域9表面は縮退し
た半導体となる。この結果、ソース領域およびド
レイン領域とのpn接合障壁の幅は非常に狭くな
り(100Å以下)、この障壁をトンネル効果で抜け
る確率が大きくなる。そして、ドレイン電圧印加
によりドレイン電流が流れるようになる。トンネ
ル電流は接合の電位差と空乏層幅に対し指数関数
的に変化するため、ドレイン電流および相互コン
ダクタンスはゲート電圧に対し強い非線形性を示
す。また、トンネル効果がこの半導体装置の基本
動作原理となつているため、電子の走行時間は非
常に短く、1ps以下である。
On the other hand, when a negative voltage is applied to the gate electrode 7 to form a hole accumulation layer on the surface of the channel region as shown in FIG. 2b, the surface of the channel region 9 becomes a degenerate semiconductor. As a result, the width of the pn junction barrier between the source region and the drain region becomes extremely narrow (100 Å or less), and the probability of tunneling through this barrier increases. Then, a drain current starts to flow by applying a drain voltage. Since tunnel current changes exponentially with junction potential difference and depletion layer width, drain current and transconductance exhibit strong nonlinearity with respect to gate voltage. Furthermore, since the tunnel effect is the basic operating principle of this semiconductor device, the transit time of electrons is extremely short, less than 1 ps.

次に、本発明の一実施例の製造方法について説
明する。
Next, a manufacturing method according to an embodiment of the present invention will be described.

まず、Siからなるp型半導体基板1表面に分子
線エピタキシ法により200Å程度チヤネル領域9
を堆積させる。次に、この表面を熱酸化して100
Å程度のゲート絶縁膜6を形成し、その上にポリ
シリコンを気相成長法により堆積させパターニン
グしてゲート電極7を形成する。
First, a channel region 9 of approximately 200 Å is formed on the surface of a p-type semiconductor substrate 1 made of Si by molecular beam epitaxy.
deposit. Next, this surface is thermally oxidized to 100%
A gate insulating film 6 having a thickness of about .ANG. is formed, and polysilicon is deposited thereon by vapor phase growth and patterned to form a gate electrode 7.

次に、このゲート電極7をマスクにp型半導体
基板1へAsのイオン注入を行ない、アニールし
てソース領域2およびドレイン領域5を形成す
る。その後、保護膜としてSiO2膜を気相成長法
により堆積し、ここにソース領域、ドレイン領域
およびゲート電極用のコンタクトホールをあけ、
Alを蒸着してそれぞれの電極形状に整形して半
導体装置を完成させる。このように、本実施例の
製造方法は非常に容易であり、高集積化に適して
いる。
Next, using gate electrode 7 as a mask, As ions are implanted into p-type semiconductor substrate 1 and annealed to form source region 2 and drain region 5. After that, a SiO 2 film was deposited as a protective film by vapor phase epitaxy, and contact holes for the source region, drain region, and gate electrode were made there.
The semiconductor device is completed by depositing Al and shaping each electrode into the shape. As described above, the manufacturing method of this embodiment is very easy and suitable for high integration.

上記実施例ではp型のチヤネル領域のものにつ
いて説明したが、本発明はそれぞれの領域の半導
体の導電型を反対にしたn型チヤネル領域のもの
に対しても同様に適用できることは明らかであ
る。また、半導体基板とチヤネル領域を同一負電
圧濃度にしてもよいが、耐圧を高め寄生容量を減
らす上からは半導体基板の不純物濃度は低くした
ほうが望ましい。もちろん、基板として絶縁物を
用いても良い。
Although the above embodiments have been described with respect to a p-type channel region, it is clear that the present invention is equally applicable to an n-type channel region in which the conductivity types of the semiconductors in each region are reversed. Furthermore, although the semiconductor substrate and the channel region may have the same negative voltage concentration, it is preferable to lower the impurity concentration of the semiconductor substrate in order to increase the withstand voltage and reduce parasitic capacitance. Of course, an insulator may be used as the substrate.

半導体としてはSiしか示さなかつたが、C,
Ge,SiC等の族半導体、GaAs,InP,InAs,
Gap,InGaAs,InGaAsP等の−族化合物半
導体、CdTe,ZnTe等の−族化合物半導体
およびその他の各種半導体でも良い。ただし、そ
れぞれの半導体で伝導帯および充満帯の状態密度
が異なつているため、縮退を生じる不純物濃度が
異なつており、本発明のソース領域およびドレイ
ン領域は充分に縮退するような高濃度の不純物を
含有しておく必要がある。また、ゲート絶縁膜と
してもSiO2以外にもSi3N4,Al2O3などの絶縁物
またはチヤネル領域の半導体よりも禁止帯幅の広
い半導体(例えばGaAsに対してAlGaAs等)を
使用しても良いことは明らかである。
Although only Si was shown as a semiconductor, C,
Group semiconductors such as Ge and SiC, GaAs, InP, InAs,
- Group compound semiconductors such as Gap, InGaAs, and InGaAsP, - group compound semiconductors such as CdTe and ZnTe, and other various semiconductors may be used. However, since the densities of states in the conduction band and charge band are different in each semiconductor, the concentration of impurities that cause degeneracy is different, and the source and drain regions of the present invention do not contain impurities at a high concentration that causes sufficient degeneration. It is necessary to contain it. In addition, insulators such as Si 3 N 4 and Al 2 O 3 other than SiO 2 can also be used as the gate insulating film, or semiconductors with a wider forbidden band width than the semiconductors in the channel region (for example, AlGaAs versus GaAs) can be used. It is clear that it is possible.

(発明の効果) 以上説明したように本発明の半導体装置は、集
積化に適した構造をもち、大きな負荷駆動能力を
有しているため、超高速動作が可能であるという
効果がある。
(Effects of the Invention) As described above, the semiconductor device of the present invention has a structure suitable for integration and has a large load driving capability, so it has the advantage of being capable of ultra-high-speed operation.

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

第1図は本発明の一実施例の断面図、第2図
a,bは第1図の実施例の熱平衡状態のバンド図
及びゲート電極に負電圧を印加したときのバンド
図、第3図は従来のMOSFETの一例の断面図、
第4図a,bは第3図のMOSFETの熱平衡状態
のバンド図及びゲート電極に正電圧を印加したと
きのバンド図である。 1……p型半導体基板、2……n型ソース領
域、3……ソース電極、4……n型ドレイン領
域、5……ドレイン電極、6……ゲート絶縁膜、
7……ゲート電極、8……チヤネル、9……p型
チヤネル領域、Ec……伝導帯端、Ev……充満帯
端、Ef……フエルミ準位。
FIG. 1 is a cross-sectional view of an embodiment of the present invention, FIGS. 2a and b are a band diagram of the embodiment in FIG. 1 in a thermal equilibrium state and a band diagram when a negative voltage is applied to the gate electrode, and FIG. 3 is a cross-sectional view of an example of a conventional MOSFET,
4a and 4b are band diagrams of the MOSFET of FIG. 3 in a thermal equilibrium state and a band diagram when a positive voltage is applied to the gate electrode. DESCRIPTION OF SYMBOLS 1...p-type semiconductor substrate, 2...n-type source region, 3...source electrode, 4...n-type drain region, 5...drain electrode, 6...gate insulating film,
7... Gate electrode, 8... Channel, 9... P-type channel region, Ec... Conduction band edge, Ev... Filling band edge, Ef... Fermi level.

Claims (1)

【特許請求の範囲】[Claims] 1 半導体または絶縁物からなる基板上に形成さ
れた一導電型の不純物を高濃度に含有し縮退状態
に近く反転層が形成されない半導体からなるチヤ
ネル領域と、該チヤネル領域を挟み前記基板上に
形成された逆導電型の高濃度不純物を含有する縮
退した半導体からなるソース領域およびドレイン
領域と、チヤネル領域の表面に設けられたゲート
電極と、前記ソース領域およびドレイン領域とそ
れぞれオーミツク接触を形成するソース電極およ
びドレイン電極とを有することを特徴とする半導
体装置。
1. A channel region formed on a substrate made of a semiconductor or an insulator and made of a semiconductor that contains impurities of one conductivity type at a high concentration and is in a degenerate state so that no inversion layer is formed, and a channel region formed on the substrate with the channel region sandwiched therebetween. a source region and a drain region made of a degenerate semiconductor containing highly concentrated impurities of opposite conductivity type; a gate electrode provided on the surface of the channel region; and a source forming ohmic contact with the source region and the drain region, respectively. A semiconductor device comprising an electrode and a drain electrode.
JP27836785A 1985-12-10 1985-12-10 Semiconductor device Granted JPS62136077A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP27836785A JPS62136077A (en) 1985-12-10 1985-12-10 Semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP27836785A JPS62136077A (en) 1985-12-10 1985-12-10 Semiconductor device

Publications (2)

Publication Number Publication Date
JPS62136077A JPS62136077A (en) 1987-06-19
JPH0546705B2 true JPH0546705B2 (en) 1993-07-14

Family

ID=17596352

Family Applications (1)

Application Number Title Priority Date Filing Date
JP27836785A Granted JPS62136077A (en) 1985-12-10 1985-12-10 Semiconductor device

Country Status (1)

Country Link
JP (1) JPS62136077A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CA1313571C (en) * 1987-10-26 1993-02-09 John W. Palmour Metal oxide semiconductor field-effect transistor formed in silicon carbide
JP2542448B2 (en) * 1990-05-24 1996-10-09 シャープ株式会社 Field effect transistor and method of manufacturing the same

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS52117587A (en) * 1976-03-30 1977-10-03 Nec Corp Insulating gate type field effect semiconductor device

Also Published As

Publication number Publication date
JPS62136077A (en) 1987-06-19

Similar Documents

Publication Publication Date Title
JP2773487B2 (en) Tunnel transistor
JP2773474B2 (en) Semiconductor device
US4471366A (en) Field effect transistor with high cut-off frequency and process for forming same
EP0114962A2 (en) Double heterojunction field effect transistors
US5391897A (en) Status induction semiconductor device
US5107314A (en) Gallium antimonide field-effect transistor
JPH0546705B2 (en)
JP2701583B2 (en) Tunnel transistor and manufacturing method thereof
JPH07142706A (en) Heterojunction semiconductor device manufacturing method and heterojunction semiconductor device
JP2800675B2 (en) Tunnel transistor
JPH088360B2 (en) Tunnel transistor and manufacturing method thereof
JPS63244779A (en) field effect transistor
JP2778447B2 (en) Tunnel transistor and manufacturing method thereof
JP3746303B2 (en) Field effect transistor
JPH025438A (en) Insulated-gate field-effect transistor
JP2710312B2 (en) Semiconductor device
JP4108252B2 (en) Electronic devices
JP2655594B2 (en) Integrated semiconductor device
JPH0362302B2 (en)
JPS60136380A (en) semiconductor equipment
JPH08148670A (en) Semiconductor device
JPH10190003A (en) Semiconductor device and manufacturing method thereof
JPH0226791B2 (en)
JPS63186479A (en) Field effect transistor
JPS63316481A (en) Field-effect semiconductor device

Legal Events

Date Code Title Description
EXPY Cancellation because of completion of term