JPH0728034B2 - Semiconductor device - Google Patents
Semiconductor deviceInfo
- Publication number
- JPH0728034B2 JPH0728034B2 JP57018618A JP1861882A JPH0728034B2 JP H0728034 B2 JPH0728034 B2 JP H0728034B2 JP 57018618 A JP57018618 A JP 57018618A JP 1861882 A JP1861882 A JP 1861882A JP H0728034 B2 JPH0728034 B2 JP H0728034B2
- Authority
- JP
- Japan
- Prior art keywords
- impurity
- containing region
- concentration
- region
- substrate
- 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
- H10D62/00—Semiconductor bodies, or regions thereof, of devices having potential barriers
- H10D62/10—Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
- H10D62/13—Semiconductor regions connected to electrodes carrying current to be rectified, amplified or switched, e.g. source or drain regions
- H10D62/149—Source or drain regions of field-effect devices
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/202—FETs having static field-induced regions, e.g. static-induction transistors [SIT] or permeable base transistors [PBT]
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 Semicon
ductor)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 Semicon) is one of the active semiconductor devices.
ductor) transistor, but it is widely used as a constituent element of an integrated circuit due to its simple structure and relatively simple manufacturing process, and the size of the element is reduced in order to highly integrate the integrated circuit. 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 shows 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 that of the substrate 1, 3 is an impurity-containing region having the same conductivity type as the impurity-containing region 2, Reference numeral 4 is an insulating film formed on the substrate 1, and 5 is a gate electrode. 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制限され
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 higher than a threshold value is applied to the gate 5 to form an inversion layer on the surface of the substrate, a large number of electrons exist in the inversion layer so that a current due to the movement of electrons flows between the source 2 and the drain. Become. 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 by the number of electrons in the layer flows. Thus, there is a weak inversion region in which the drain current changes with the change of the gate voltage.
第2図は従来構造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。MOS
トランジスタが微細化され、動作電圧が低くなると、弱
反転領域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。したがって弱反転領域b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。Figure 2 shows the gate voltage (V G ) of a conventional MOS transistor.
It is a weak inversion characteristic of the drain current (log Ib) with respect to.
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. MOS
When the transistor is miniaturized and the operating voltage is lowered, the weak inversion region b is not narrowed, so that the operating margin of each region of a and c is narrowed. Therefore, it is extremely effective if the characteristic (dotted line) where the weak inversion region b does not exist can be realized.
本発明の目的は、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な半導体装置を提供することにあ
る。An object of the present invention is to eliminate the drawbacks of the conventional MOS transistor and to provide a novel semiconductor device based on a new operation principle capable of high speed operation and high density.
本発明によれば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型で急峻な不純物分布を有する
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
電型を有する第2の高濃度不純物含有領域と、前記第1
と第2の高濃度不純物含有領域との間の半導体基板表面
に絶縁膜を介して設けられた電極と、少くとも前記半導
体基板表面の一部において該電極下の第2の高濃度不純
物含有領域と前記半導体基板との境界線を含み、該境界
線から離れるに従い不純物濃度が第2の高濃度不純物含
有領域と同程度の不純物濃度からゆるやかに減少してい
る第2の高濃度不純物含有領域と同型の不純物含有領域
とで構成されており、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の縮退した高濃度不純物領
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
装置が得られる。According to the present invention, a semiconductor substrate and a first degenerated high-concentration impurity-containing region which is provided in a part of the semiconductor substrate surface and has the same type and a steep impurity distribution as the substrate, and another one of the semiconductor substrate surface. A second high-concentration impurity-containing region having a second conductivity type different from that of the substrate, and the first
And an electrode provided on the surface of the semiconductor substrate via an insulating film between the second high-concentration impurity-containing region and a second high-concentration impurity-containing region below the electrode on at least a part of the semiconductor substrate surface. And a second high-concentration impurity-containing region in which the impurity concentration gradually decreases from the same level as the second high-concentration impurity-containing region as the distance from the boundary line increases. A semiconductor device characterized by controlling a tunnel current between a high-concentration carrier region formed on the surface of a semiconductor substrate below an electrode and a first degenerated high-concentration impurity region, which is formed of an impurity-containing region of the same type. can get.
前記本発明は、基板表面に設けられたp-n接合の空乏層
の厚さをこの接合上に設けたゲート電極により変化さ
せ、この接合間を流れるトンネル電流を制御するという
動作原理に基づく新規な半導体装置である。The present invention is a novel semiconductor based on the operation principle that the thickness of the depletion layer of the pn junction provided on the substrate surface is changed by the gate electrode provided on this junction to control the tunnel current flowing between the junctions. It is a device.
以下本発明について実施例を示す図面を参照して詳細に
説明する。Hereinafter, the present invention will be described in detail with reference to the drawings illustrating an embodiment.
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半導体基板、
12は該基板11と同じ導電型で急峻な不純物分布を有する
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と異る導電型を有する第2の高濃度不純
物含有領域、14は該高濃度不純物含有領域13を含む領域
に設けられ当該高濃度不純物含有領域13から離れるに従
い不純物濃度が当該高濃度不純物含有領域13と同じ不純
物濃度からゆるやかに減少している当該高濃度不純物含
有領域13と同型の不純物含有領域である。2つの高濃度
不純物含有領域12,13の不純物濃度は1×1019cm-3以上
であり、第1の高濃度不純物含有領域12と基板11との接
合における不純物濃度分布はステップ状であることが望
ましい。基板11表面に拡散定数の小さい砒素等のイオン
をイオンインプランテーションすれば、表面濃度1×10
21cm-3で接合深さ0.3μmのほぼステップとみなせる接
合が完成する。なお、2つの高濃度不純物含有領域12,1
3はそれぞれソース,ドレインと呼ぶ。また、不純物含
有領域14の不純物濃度がゆるやかに変化している領域の
長さは0.1μm以上であることが望ましい。不純物含有
領域14はソース,ドレイン形成前にドレイン部に拡散定
数の大きいリン等のイオンをイオンインプランテーショ
ンし、熱処理で傾斜接合を作ることにより実現できる。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 semiconductor substrate having one conductivity type,
Reference numeral 12 denotes a first degenerate high-concentration impurity-containing region having the same conductivity type as that of the substrate 11 and having a steep impurity distribution, and 13 denotes a second high-concentration impurity-containing region having a conductivity type different from that of the high-concentration impurity-containing region 12. The region, 14 is provided in a region including the high-concentration impurity-containing region 13, and the impurity concentration gradually decreases from the same impurity concentration as the high-concentration impurity-containing region 13 as the distance from the high-concentration impurity-containing region 13 increases. This is an impurity-containing region of the same type as the concentration impurity-containing region 13. The impurity concentration of the two high-concentration impurity-containing regions 12 and 13 is 1 × 10 19 cm −3 or more, and the impurity concentration distribution at the junction between the first high-concentration impurity-containing region 12 and the substrate 11 is step-shaped. Is desirable. If ions such as arsenic having a small diffusion constant are ion-implanted on the surface of the substrate 11, the surface concentration is 1 × 10.
At 21 cm -3 , a joint with a joint depth of 0.3 μm that can be regarded as a step is completed. Two high-concentration impurity-containing regions 12,1
3 are called source and drain, respectively. Further, the length of the region where the impurity concentration of the impurity-containing region 14 is gradually changed is preferably 0.1 μm or more. The impurity-containing region 14 can be realized by ion-implanting phosphorus or other ions having a large diffusion constant in the drain portion before forming the source and drain, and forming a graded junction by heat treatment.
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。簡単のため、半導体基板
11の表面は熱平衡状態でフラットバンド状態になってい
るとする。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接合が逆バイアスとなるよう
ソース12をアース電位とし、ドレイン13が正電位となる
ようにかける。なお、基板11はソースとP-P+接合を作っ
ているので、その電位はほぼアース電位に設定される。
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ア領域が形成されて
いないとすると、基板11とドレイン13の回りの不純物含
有領域14とのp-n接合において厚い空乏層が基板11およ
び不純物含有領域14内に形成されるので、ソース12とド
レイン13との間を電流(ドレイン電流)は流れない。一
方、ゲート電極5にしきい値電圧より高い正電圧を印加
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、基板表面における該
反転層とソース12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に充分大きな負電圧を印加
し、基板表面に高濃度の正孔の蓄積層を形成すると、該
蓄積層とソース12とは接続され、基板表面における接合
はドレイン13およびこの回りの不純物含有領域14と前記
蓄積層との間に形成されるが、厚い空乏層が不純物含有
領域14内に広がるため、ソース12とドレイン13との間に
電流は流れない。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. Semiconductor substrate for simplicity
It is assumed that the surface of 11 is in a flat band state in thermal equilibrium. The bias voltage (drain voltage) between the source 12 and the drain 13 is applied so that the source 12 is at the ground potential and the drain 13 is at the positive potential so that the pn junction is reverse biased. Since the substrate 11 forms a PP + junction with the source, its potential is set to approximately ground potential.
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, the pn junction between the substrate 11 and the impurity-containing region 14 around the drain 13 is formed. At, a thick depletion layer is formed in the substrate 11 and the impurity-containing region 14, so that no current (drain current) flows between the source 12 and the drain 13. On the other hand, when a positive 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 inversion layer and the source on the substrate surface are connected. The junction with 12 is an equivalent P + -n + tunnel junction, the depletion layer on the surface is almost not spread, 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. Further, 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 accumulation layer and the source 12 are connected, and the junction on the substrate surface forms the drain 13 and the surrounding area. Although it is formed between the impurity-containing region 14 and the storage layer, no current flows between the source 12 and the drain 13 because the thick depletion layer spreads in the impurity-containing region 14. 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、従来MOSト
ランジスタと同様に動作がゲート電圧に関して単極性で
あり、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等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, the operation is unipolar with respect to the gate voltage as in the conventional MOS transistor, and no current flows until carrier tunneling occurs, resulting in a weak voltage as shown in FIG. 2 (b). There is no inversion region, and a characteristic close to the ideal characteristic (dotted line) in FIG. 2 is 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 an equivalent resistor of the active device in series.
第4図は本発明の他の一実施例を示す断面模式図であ
る。第4図において第1図および第3図と同じ番号のも
のは第1図および第3図と同等物で同一機能を示す。15
は高濃度不純物含有領域13に接し、ゲート電極5の下の
基板11の表面に設けられ、前記高濃度不純物含有領域13
から離れるに従い不純物濃度が当該高濃度不純物含有領
域13と同じ不純物濃度からゆるやかに減少している当該
高濃度不純物含有領域13と同型の不純物含有領域であ
る。該不純物含有領域15は、例えば不純物イオンをドレ
イン側からゲート電極下の基板表面方向に斜めにイオン
注入し、ゲート電極下にゆるやかな接合を形成すること
によって実現できる。なお、ゲート電極が不純物含有領
域15の一部の上までしかなく、ドレイン13上にない場
合、ソース側でトンネル現象が起こっても、ゲート電極
が該不純物領域15の上部に存在しない場所では電流が流
れにくくなるため、あまり好ましくない。FIG. 4 is a schematic sectional view showing another embodiment of the present invention. In FIG. 4, the same reference numerals as those in FIGS. 1 and 3 are equivalent to those in FIGS. 1 and 3 and show the same functions. 15
Is provided on the surface of the substrate 11 below the gate electrode 5 in contact with the high-concentration impurity-containing region 13, and the high-concentration impurity-containing region 13 is provided.
The impurity concentration region is the same type as the high concentration impurity concentration region 13 in which the impurity concentration gradually decreases from the same impurity concentration as the high concentration impurity concentration region 13. The impurity-containing region 15 can be realized, for example, by implanting impurity ions obliquely from the drain side in the direction of the substrate surface under the gate electrode to form a loose junction under the gate electrode. Note that when the gate electrode is present only above a part of the impurity-containing region 15 and not above the drain 13, even if a tunnel phenomenon occurs on the source side, the current does not flow in a place where the gate electrode does not exist above the impurity region 15. Is difficult to flow, which is not preferable.
該不純物含有領域15は素子の動作においては前記の第3
図の不純物含有領域14と同一機能を持つものであるか
ら、本実施例の動作原理および動作上の特徴は第3図で
示した本発明の実施例と同一である。The impurity-containing region 15 is the above-mentioned third region in the operation of the device.
Since it has the same function as the impurity-containing region 14 in the figure, the operating principle and operational characteristics of this embodiment are the same as those of the embodiment of the present invention shown in FIG.
以上、本発明による新規半導体装置の構造および動作に
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は明ら
かである。Although the structure and operation of the novel semiconductor device according to the present invention have been described above by using the P-type substrate, it is obvious that the same effect can be achieved when the substrate is the n-type. Further, it is obvious that the novel semiconductor device according to the present invention can be realized even if the semiconductor substrate is replaced by a thin film or thick film semiconductor.
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と異なる
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図と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で急峻
な不純物分布を有する第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の高濃度不純物含有領域、14は該高濃
度不純物含有領域13を含む領域に設けられた当該高濃度
不純物含有領域13から離れるに従い不純物濃度が当該高
濃度不純物含有領域13と同程度の不純物濃度からゆるや
かに減少している当該高濃度不純物含有領域13と同型の
不純物領域である。 第4図は本発明の他の一実施例を示す断面模式図であ
り、第1図および第3図と同じ番号のものは第1図およ
び第3図と同等物で同一機能を示し、15は高濃度不純物
含有領域13に接しゲート電極5の下の基板11の表面に設
けられ、前記高濃度不純物含有領域13から離れるに従い
不純物濃度が当該高濃度不純物領域13と同程度の不純物
濃度からゆるやかに減少している当該高濃度不純物含有
領域13と同型の不純物含有領域である。FIG. 1 is a schematic diagram of a conventional structure MOS transistor.
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 on the substrate 1. The formed insulating films 5 are gate electrodes. Figure 2 shows the weak inversion characteristics of the drain current with respect to the drain voltage of the conventional structure MOS transistor. The solid line shows the conventional structure.
The characteristics of the MOS transistor, the dotted line is the characteristics of the ideal switching transistor, a is the region where the junction leak current of the source and drain flows, b is the weak inversion region, V T is the threshold voltage, and c is the strong inversion region. FIG. 3 is a schematic sectional view showing an embodiment of the present invention, in which the same reference numerals as those in FIG. 1 are equivalent and indicate 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 a steep impurity distribution, 13 is a second high-concentration impurity-containing region having a second conductivity type different from the high-concentration impurity-containing region 12, 14 Indicates that the impurity concentration gradually decreases from the same impurity concentration as the high-concentration impurity-containing region 13 as the distance from the high-concentration impurity-containing region 13 provided in the region including the high-concentration impurity-containing region 13 increases. This is an impurity region of the same type as the concentration impurity-containing region 13. FIG. 4 is a schematic cross-sectional view showing another embodiment of the present invention, in which the same reference numerals as those in FIGS. 1 and 3 are equivalent to those in FIGS. 1 and 3 and show the same function. Is provided on the surface of the substrate 11 below the gate electrode 5 in contact with the high-concentration impurity-containing region 13, and as the distance from the high-concentration impurity-containing region 13 increases, the impurity concentration gradually changes from the same impurity concentration as that of the high-concentration impurity region 13. It is an impurity-containing region of the same type as that of the high-concentration impurity-containing region 13 that has decreased to 1.
Claims (1)
設けられた当該基板と同型で急峻な不純物分布を有する
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なる第2の
導電型を有する第2の高濃度不純物含有領域と前記第1
と第2の高濃度不純物含有領域との間の半導体基板表面
に絶縁膜を介して設けられた電極と、少なくとも前記半
導体基板表面の一部において該電極下の第2の高濃度不
純物含有領域と前記半導体基板との境界線を含み、該境
界線から離れるに従い不純物濃度が第2の高濃度不純物
含有領域と同程度の不純物濃度からゆるやかに減少して
いる第2の高濃度不純物含有領域と同型の不純物含有領
域とで構成されており、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 having the same type and a steep impurity distribution as that of the substrate, which is provided on a part of the surface of the semiconductor substrate, and another surface of the semiconductor substrate. A second high-concentration impurity-containing region having a second conductivity type different from that of the substrate and provided in a part of the first substrate;
An electrode provided on the surface of the semiconductor substrate via an insulating film between the second high-concentration impurity-containing region and a second high-concentration impurity-containing region below the electrode at least at a part of the semiconductor substrate surface. The same concentration as the second high-concentration impurity-containing region, which includes the boundary with the semiconductor substrate, and whose impurity concentration gradually decreases from the same level as the second high-concentration impurity-containing region as the distance from the boundary increases. And a tunnel current between the high-concentration carrier region formed on the surface of the semiconductor substrate below the electrode and the first degenerated high-concentration impurity-containing region.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57018618A JPH0728034B2 (en) | 1982-02-08 | 1982-02-08 | Semiconductor device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57018618A JPH0728034B2 (en) | 1982-02-08 | 1982-02-08 | Semiconductor device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58135673A JPS58135673A (en) | 1983-08-12 |
| JPH0728034B2 true JPH0728034B2 (en) | 1995-03-29 |
Family
ID=11976604
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57018618A Expired - Lifetime JPH0728034B2 (en) | 1982-02-08 | 1982-02-08 | Semiconductor device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0728034B2 (en) |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS52115671A (en) * | 1977-01-21 | 1977-09-28 | Agency Of Ind Science & Technol | Multi-terminal type semiconductor element |
-
1982
- 1982-02-08 JP JP57018618A patent/JPH0728034B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58135673A (en) | 1983-08-12 |
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