JPH0612821B2 - Semiconductor device - Google Patents
Semiconductor deviceInfo
- Publication number
- JPH0612821B2 JPH0612821B2 JP56194992A JP19499281A JPH0612821B2 JP H0612821 B2 JPH0612821 B2 JP H0612821B2 JP 56194992 A JP56194992 A JP 56194992A JP 19499281 A JP19499281 A JP 19499281A JP H0612821 B2 JPH0612821 B2 JP H0612821B2
- Authority
- JP
- Japan
- Prior art keywords
- substrate
- drain
- region
- impurity
- junction
- 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
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]
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D12/00—Bipolar devices controlled by the field effect, e.g. insulated-gate bipolar transistors [IGBT]
- H10D12/211—Gated diodes
Landscapes
- Insulated Gate Type Field-Effect Transistor (AREA)
- Bipolar Transistors (AREA)
Description
【発明の詳細な説明】 本発明は高速度動作の可能な新規半導体装置の構造に関
するものである。The present invention relates to the structure of a novel semiconductor device capable of high speed operation.
能動半導体装置の1つとしてMOS(Metal Oxide Semi
conductor)トランジスタがあるが、その構造の単純性
及び製造プロセスが比較的簡単なことにより、集積回路
の構成素子として広く用いられており、集積回路を高集
積化すべく素子寸法の縮小が計られ、また動作の高速化
が計られている。MOS (Metal Oxide Semi) is one of the active semiconductor devices.
conductor) transistor, it is widely used as a constituent element of an integrated circuit because of its simple structure and relatively simple manufacturing process, and the size of the element is reduced in order to make the integrated circuit highly integrated. In addition, the speed of operation is being measured.
第1図に従来構造のMOSトランジスタの概略構造及び
動作を説明する模式図を示す。第1図において1は一導
電型を有する半導体基板、2は該基板1と異る第2の導
電型を有する不純物含有領域、3は該不純物含有領域2
と同じ導電型を有する不純物含有領域、4は基板1の上
に形成された絶縁膜、5はゲート電極である。なお、電
気回路における表現では不純物含有領域2はソース、不
純物含有領域3はドレイン電極、5はゲート電極と呼ば
れている。FIG. 1 is a schematic diagram for explaining the schematic structure and operation of a conventional MOS transistor. In FIG. 1, 1 is a semiconductor substrate having one conductivity type, 2 is an impurity-containing region having a second conductivity type different from the substrate 1, and 3 is an impurity-containing region 2.
Impurity containing regions having the same conductivity type as 4 are insulating films formed on the substrate 1, and 5 are gate electrodes. In the expression in the electric circuit, the impurity-containing region 2 is called a source, the impurity-containing region 3 is called a drain electrode, and 5 is called a gate electrode.
半導体基板1にP型を用いてこのMOSトランジスタの
動作を説明すると次のようになる。基板1とソース2を
零電位とし、ドレイン3には正電圧が印加されている。
いま、ゲート5に負の電圧を加え基板表面に反転層が形
成されないようにすると、ソース2とドレイン3との間
の半導体基板1の表面にはソース及びドレインにおける
多数キャリアである電子がほとんど存在しないため、ソ
ース2とドレイン3との間には電流は流れない。さて、
ゲート5にしきい値以上の正電圧を加え基板表面に反転
層を形成すると、反転層内には電子が多数存在するため
ソース2とドレインとの間は電子の移動による電流が流
れるようになる。しかし、この2つの状態はステップ状
に変わるのではなくゲート電圧がしきい値近傍である場
合には基板表面には弱い反転層が形成され、ソース2と
ドレイン3との間には該反転層内の電子の数に限定され
た電流(ドレイン電流)が流れる。このように、ドレイ
ン電流がゲート電圧の変化と共に変化する弱反転領域が
存在する。The operation of this MOS transistor using the P type semiconductor substrate 1 will be described below. The substrate 1 and the source 2 are set to zero potential, and a positive voltage is applied to the drain 3.
Now, if a negative voltage is applied to the gate 5 so that the inversion layer is not formed on the substrate surface, most of the electrons, which are majority carriers in the source and drain, exist on the surface of the semiconductor substrate 1 between the source 2 and the drain 3. Therefore, no current flows between the source 2 and the drain 3. Now,
When a positive voltage above the threshold is applied to the gate 5 to form an inversion layer on the surface of the substrate, a large number of electrons are present in the inversion layer, so that a current flows due to the movement of electrons between the source 2 and the drain. However, these two states do not change stepwise, but when the gate voltage is near the threshold value, a weak inversion layer is formed on the substrate surface, and the inversion layer is formed between the source 2 and the drain 3. A current (drain current) limited to the number of electrons inside flows. Thus, there is a weak inversion region in which the drain current changes with the change of the gate voltage.
第2は従来構造MOSトランジスタのゲート電圧(VG)に
対するドレイン電流(log Ib)の弱反転特性である。第
2図において実線は従来構造MOSトランジスタの特
性、点線は理想的なスイッチングトランジスタの特性、
aはソース2およびドレイン3の接合におけるリーク電
流が流れる領域、bは弱反転領域、VTはしきい値電圧、
cは大きなドレイン電流が流れ得る反転層が形成されて
いる強反転領域である。スイッチング動作としてはaと
cの二領域を用いるだけでbは本質的には不要である。
しかし、実際上これを除去することは困難である。MO
Sトランジスタが微細化され、動作電圧が低くなると、
遷移領域bは狭くならないためにaとcの各領域の動作
マージンが狭くなる。したがって遷移領域の存在しない
特性(点線)が実現できれば極めて有効である。The second is the weak inversion characteristic of the drain current (log Ib) with respect to the gate voltage (V G ) of the conventional structure MOS transistor. In FIG. 2, the solid line is the characteristic of the conventional structure MOS transistor, the dotted line is the characteristic of the ideal switching transistor,
a is a region where a leak current flows at the junction of the source 2 and the drain 3, b is a weak inversion region, V T is a threshold voltage,
c is a strong inversion region in which an inversion layer through which a large drain current can flow is formed. Only two regions a and c are used for the switching operation, and b is essentially unnecessary.
However, it is practically difficult to remove it. MO
When the S transistor is miniaturized and the operating voltage becomes low,
Since the transition region b is not narrowed, the operation margin of each region of a and c is narrowed. Therefore, it is extremely effective if the characteristic (dotted line) without the transition region can be realized.
本発明は、かかる従来のMOSトランジスタの持つ欠点
を除去し、高速動作及び高密度化が可能な新しい動作原
理に基づく新規半導体装置を提供するものである。The present invention eliminates the drawbacks of the conventional MOS transistor and provides a new semiconductor device based on a new operation principle that enables high-speed operation and high density.
その要旨は、半導体基板と、該半導体基板表面の一部に
設けられた当該基板と同じ導電型で基板との接合におけ
る不純物分布が急峻な第1の縮退した高濃度不純物含有
領域と、前記半導体基板表面の他の一部に設けられた当
該基板と異る第2の導電型を有し基板との接合における
不純物分布が急峻な第2の縮退した高濃度不純物含有領
域と、前記第1と第2の縮退した高濃度不純物含有領域
との間の半導体基板上全体に絶縁膜を介して設けられた
ゲート電極とからなり、該ゲート電極下の半導体基板表
面に形成する高濃度キャリア領域と第1または第2の縮
退した高濃度不純物含有領域間のトンネル電流を制御す
る半導体装置を提供するものである。この半導体装置に
おいてはゲート電極にかける電圧によって、第1と第2
の高濃度不純物領域との間に流れるトンネル電流を制御
し、従来構造のような繊維領域を持たない特性を実現す
ることが可能となる。The gist thereof is that a semiconductor substrate, a first degenerate high-concentration impurity-containing region that is provided on a part of the surface of the semiconductor substrate, has the same conductivity type as the substrate, and has a sharp impurity distribution at the junction with the substrate; A second degenerate high-concentration impurity-containing region that is provided on another part of the substrate surface and has a second conductivity type different from that of the substrate and has a steep impurity distribution at the junction with the substrate; A high-concentration carrier region formed on the surface of the semiconductor substrate below the gate electrode, and a gate electrode provided on the entire semiconductor substrate between the second degenerated high-concentration impurity-containing region and an insulating film. A semiconductor device for controlling a tunnel current between the first or second degenerate high-concentration impurity-containing regions. In this semiconductor device, depending on the voltage applied to the gate electrode, the first and second
It is possible to control the tunnel current flowing between the high-concentration impurity region and the high-concentration impurity region, and to realize the characteristic that the conventional structure does not have the fiber region.
以下本発明の動作原理を実施例図面を参照して詳細に説
明する。Hereinafter, the operating principle of the present invention will be described in detail with reference to the accompanying drawings.
第3図は本発明の一実施例を示す断面模式図である。第
3図において第1図と同じ番号のものは第1図と同等物
で同一機能を示す。11は一導電型を有する基板、12は該
基板11と同じ導電性を有する第1の縮退した高濃度不純
物含有領域、13は該高濃度不純物含有領域12とは異る第
2の導電型を有する第2の縮退した高濃度不純物含有領
域である。2つの縮退した高濃度不純物含有領域12、13
の基板1との接合における不純物濃度は1×1019cm-3以
上でその分布はステップ状であることが望ましい。この
実現は容易ではないが、基板1表面に拡散定数の小さい
砒素をイオンインプランテーションして接合を作る場
合、表面濃度1×1021cm-3で接合深さ0.3μmであれば
ほぼこの条件を満足する。なお、2つの縮退した高濃度
不純物含有領域12、13はそれぞれソース、ドレインと呼
ぶ。FIG. 3 is a schematic sectional view showing an embodiment of the present invention. In FIG. 3, those having the same numbers as in FIG. 1 are equivalent to those in FIG. 1 and show the same functions. 11 is a substrate having one conductivity type, 12 is a first degenerate high-concentration impurity-containing region having the same conductivity as the substrate 11, and 13 is a second conductivity type different from the high-concentration impurity-containing region 12. The second degenerate high-concentration impurity-containing region has. Two degenerated high-concentration impurity-containing regions 12 and 13
It is desirable that the impurity concentration at the junction with the substrate 1 of 1 × 10 19 cm −3 or more and the distribution thereof be stepwise. This is not easy to realize, but when arsenic having a small diffusion constant is ion-implanted on the surface of the substrate 1 to form a junction, this condition is almost satisfied if the surface concentration is 1 × 10 21 cm −3 and the junction depth is 0.3 μm. Be satisfied. The two degenerated high-concentration impurity-containing regions 12 and 13 are called a source and a drain, respectively.
半導体基板11にP型を用いてこの新規半導体装置の動作
を説明すると次のようになる。ソース12とドレイン13の
間のバイアス電圧(ドレイン電圧)は、p−nの接合が
逆バイアスとなるようソース12は零電位、ドレイン13が
正電圧となっている。なお、基板1は電極を接続しない
がその電位はほぼソース12の電位で決まる。いま、ゲー
ト電極5の電圧の絶対値が小さく、基板表面に蓄積層又
は反転層の高濃度キャリヤ領域が形成されてないとする
と、基板11とドレイン13とのp−n+接合において厚い空
乏層が基板11内に形成されるので、ソース12とドレイン
13の間を電流(ドレイン電流)は流れない。一方、ゲー
ト電極5に充分に大きい負電圧を印加し、基板表面に高
濃度の正孔蓄積層を形成すると、基板表面における該蓄
積層とドレイン13との接合は等価的なp+−n+トンネル接
合となり、表面における空乏層はほとんど広がらず、こ
の接合は高電界となる。この空乏層の幅が数十Å以下と
なるとこの空乏層内をキャリアはトンネルで通過でき、
ソース12とドレイン13の間にトンネル電流が流れるよう
になる。またゲート電極5にしきい値電圧より高い電圧
を印加し、基板表面に高濃度の電子の反転層を形成する
と、該反転層とドレイン13とは接続され、基板表面にお
ける接合はソース12と前記反転層との間に形成され等価
的なp++n+トンネル接合となり、表面における空乏層は
ほとんど広がらずこの接合は高電界となる。この結果、
該接合において前述の蓄積層とドレイン13との接合と同
様キャリアのトンネルが起こり、ソース12とドレイン13
の間にトンネル電流が流れるようになる。このようにゲ
ート電圧によりドレイン電流を制御することができる。The operation of this new semiconductor device using the P type semiconductor substrate 11 is as follows. Regarding the bias voltage (drain voltage) between the source 12 and the drain 13, the source 12 has a zero potential and the drain 13 has a positive voltage so that the pn junction has a reverse bias. It should be noted that the substrate 1 has no electrodes connected thereto, but its potential is almost determined by the potential of the source 12. Now, assuming that the absolute value of the voltage of the gate electrode 5 is small and the high-concentration carrier region of the accumulation layer or the inversion layer is not formed on the substrate surface, a thick depletion layer is formed in the pn + junction between the substrate 11 and the drain 13. Are formed in the substrate 11 so that the source 12 and drain
A current (drain current) does not flow between 13's. On the other hand, when a sufficiently large negative voltage is applied to the gate electrode 5 to form a high concentration hole accumulation layer on the substrate surface, the junction between the accumulation layer and the drain 13 on the substrate surface is equivalent to p + -n + It becomes a tunnel junction, the depletion layer on the surface hardly spreads, and this junction has a high electric field. When the width of this depletion layer becomes several tens of liters or less, carriers can pass through this depletion layer by a tunnel,
A tunnel current comes to flow between the source 12 and the drain 13. When a voltage higher than the threshold voltage is applied to the gate electrode 5 to form a high-concentration electron inversion layer on the substrate surface, the inversion layer and the drain 13 are connected, and the junction on the substrate surface is the source 12 and the inversion. An equivalent p + + n + tunnel junction is formed between the layer and the layer, and the depletion layer on the surface hardly spreads, and this junction has a high electric field. As a result,
At the junction, a carrier tunnel occurs as in the junction between the storage layer and the drain 13 described above, and the source 12 and the drain 13 are tunneled.
The tunnel current comes to flow between. In this way, the drain current can be controlled by the gate voltage.
本発明はこのような原理によっているため、キャリアの
トンネルが起こるまでは全く電流が流れず、第2図bの
ような弱反転領域は存在せず、第2図の理想特性(点
線)に近い特性が得られる。ただし、本発明による半導
体装置では素子の導通状態で電流を制限する機構が無い
ので、この電流制限のための抵抗、又は能動デバイスの
特価的な抵抗を直列に入れておくのが望ましい。Since the present invention is based on such a principle, no current flows until carrier tunneling occurs, and there is no weak inversion region as shown in FIG. 2b, which is close to the ideal characteristic (dotted line) in FIG. The characteristics are obtained. However, since the semiconductor device according to the present invention does not have a mechanism for limiting the current in the conductive state of the element, it is desirable to insert a resistor for limiting the current or a special-priced resistor for the active device in series.
本発明による新規半導体装置においては微細化及び高速
化が計れる可能性を有するが、この他に従来の能動半導
体装置にないいくつかの特徴を有している。第1は動作
がゲート電圧に関して両極性であることであり、第2は
基板の導電型によらず同一プロセスで形成できることで
あり、第3はドレイン電流がトンネル効果により電流が
流れるため、ドレイン電圧に対するドレイン電流の特性
は非飽和特性であることである。The novel semiconductor device according to the present invention has a possibility of achieving miniaturization and high speed, but has some other features which are not present in the conventional active semiconductor device. The first is that the operation is bipolar with respect to the gate voltage, the second is that it can be formed in the same process regardless of the conductivity type of the substrate, and the third is that the drain current flows due to the tunnel effect, so the drain voltage The characteristic of the drain current with respect to is that it is a non-saturation characteristic.
以上、本発明による新規半導体装置の構造及び動作につ
いてp型基板を用いて説明してきたが、基板をn型にし
た場合も同様に実現できることは明らかである。また、
半導体基板の替りに薄膜又は厚膜半導体で構成しても本
発明による新規半導体装置が実現できることも明らであ
る。Although the structure and operation of the novel semiconductor device according to the present invention have been described above using the p-type substrate, it is obvious that the same can be realized when the substrate is an n-type. Also,
It is also clear that the novel semiconductor device according to the present invention can be realized by using a thin film or thick film semiconductor instead of the semiconductor substrate.
第1図は従来構造MOSトランジスタの模式図であり、
1は一導電型を有する半導体基板、2は該基板1と異る
第2の導電型を有する不純物含有領域、3は該不純物含
有領域2と同じ極性を有する不純物含有領域、4は基板
1の上に形成された絶縁膜、5はゲート電極である。 第2図は従来構造MOSトランジスタのドレイン電圧に
対するドレイン電流の弱反転特性であり、実線は従来構
造MOSトランジスタの特性、点線は理想的なスイッチ
ングトランジスタの特性、aはソースおよびドレインの
接合リーク電流の流れる領域、bは弱反転領域、VTは
しきい値電圧、cは強反転領域である。 第3図は本発明の一実施例を示す断面模式図であり、第
1図の同じ番号のものは同等物で同一機能を示し、11は
一導電型を有する基板、12は該基板と同じ導電型を有す
る第1の縮退した高濃度不純物含有領域、13は該高濃度
不純物含有領域12とは異る第2の導電型を有する第2の
縮退した高濃度不純物領域である。FIG. 1 is a schematic view of a conventional structure MOS transistor,
1 is a semiconductor substrate having one conductivity type, 2 is an impurity-containing region having a second conductivity type different from that of the substrate 1, 3 is an impurity-containing region having the same polarity as the impurity-containing region 2, and 4 is a substrate 1. The insulating films 5 formed on the gate electrodes are gate electrodes. FIG. 2 shows the weak inversion characteristic of the drain current with respect to the drain voltage of the conventional structure MOS transistor, the solid line shows the characteristic of the conventional structure MOS transistor, the dotted line shows the characteristic of the ideal switching transistor, and a is the junction leak current of the source and drain. A flowing region, b is a weak inversion region, V T is a threshold voltage, and c is a strong inversion region. FIG. 3 is a schematic cross-sectional view showing an embodiment of the present invention, in which the same numbers in FIG. 1 are equivalent and show the same function, 11 is a substrate having one conductivity type, 12 is the same as the substrate. A first degenerate high-concentration impurity-containing region having a conductivity type, and 13 is a second degenerate high-concentration impurity-containing region having a second conductivity type different from the high-concentration impurity-containing region 12.
Claims (1)
設けられた当該基板と同じ導電型で基板との接合におけ
る不純物分布が急峻な第1の縮退した高濃度不純物含有
領域と、前記半導体基板表面の他の一部に設けられた当
該基板と逆導電型で基板との接合における不純物分布が
急峻な第2の縮退した高濃度不純物含有領域と、前記第
1と第2の縮退した高濃度不純物含有領域との間の半導
体基板上全体に絶縁膜を介して設けられた電極とからな
り、該電極下の半導体基板表面に形成する高濃度キャリ
ア領域と第1または第2の縮退した高濃度不純物含有領
域間のトンネル電流を制御することを特徴とする半導体
装置。1. A semiconductor substrate, a first degenerate high-concentration impurity-containing region which is provided on a part of the surface of the semiconductor substrate, has the same conductivity type as the substrate, and has a sharp impurity distribution at the junction with the substrate. A second degenerate high-concentration impurity-containing region, which is provided on another part of the surface of the semiconductor substrate, has a conductivity type opposite to that of the substrate and has a steep impurity distribution at the junction with the substrate, and the first and second degenerate regions. A high-concentration carrier region formed on the surface of the semiconductor substrate below the electrode, and the first or second degenerated region. A semiconductor device characterized by controlling a tunnel current between high-concentration impurity-containing regions.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56194992A JPH0612821B2 (en) | 1981-12-03 | 1981-12-03 | Semiconductor device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56194992A JPH0612821B2 (en) | 1981-12-03 | 1981-12-03 | Semiconductor device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5896766A JPS5896766A (en) | 1983-06-08 |
| JPH0612821B2 true JPH0612821B2 (en) | 1994-02-16 |
Family
ID=16333730
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56194992A Expired - Lifetime JPH0612821B2 (en) | 1981-12-03 | 1981-12-03 | Semiconductor device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0612821B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0425175A (en) * | 1990-05-21 | 1992-01-28 | Canon Inc | Diode |
| JP2701583B2 (en) * | 1991-03-05 | 1998-01-21 | 日本電気株式会社 | Tunnel transistor and manufacturing method thereof |
| JP2773474B2 (en) * | 1991-08-06 | 1998-07-09 | 日本電気株式会社 | Semiconductor device |
-
1981
- 1981-12-03 JP JP56194992A patent/JPH0612821B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5896766A (en) | 1983-06-08 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JP2773487B2 (en) | Tunnel transistor | |
| JP2773474B2 (en) | Semiconductor device | |
| US4009483A (en) | Implementation of surface sensitive semiconductor devices | |
| US4458261A (en) | Insulated gate type transistors | |
| US4839703A (en) | High speed and power transistor | |
| JPH02307274A (en) | Semiconductor device | |
| JPH0612821B2 (en) | Semiconductor device | |
| US4910562A (en) | Field induced base transistor | |
| US3493824A (en) | Insulated-gate field effect transistors utilizing a high resistivity substrate | |
| JPS5921170B2 (en) | MOS type semiconductor device | |
| US5331194A (en) | Bipolar static induction transistor | |
| US4829349A (en) | Transistor having voltage-controlled thermionic emission | |
| JPS6123669B2 (en) | ||
| US3500138A (en) | Bipolar mos field effect transistor | |
| JPH0411780A (en) | Insulated gate type bipolar transistor | |
| JPS6241428B2 (en) | ||
| JPH0359579B2 (en) | ||
| JPH01238062A (en) | Anode short type conductive modulation mosfet | |
| JP2608976B2 (en) | Semiconductor device | |
| JPH0728035B2 (en) | Semiconductor device | |
| US5416339A (en) | Semiconductor device having electrode for collecting electric charge in channel region | |
| JPS6349392B2 (en) | ||
| JPH0728034B2 (en) | Semiconductor device | |
| KR100192966B1 (en) | Mos control diode and manufacturing method thereof | |
| JPH07106581A (en) | Semiconductor device |