JPH0353788B2 - - Google Patents
Info
- Publication number
- JPH0353788B2 JPH0353788B2 JP57046705A JP4670582A JPH0353788B2 JP H0353788 B2 JPH0353788 B2 JP H0353788B2 JP 57046705 A JP57046705 A JP 57046705A JP 4670582 A JP4670582 A JP 4670582A JP H0353788 B2 JPH0353788 B2 JP H0353788B2
- Authority
- JP
- Japan
- Prior art keywords
- insulating film
- field effect
- effect transistor
- avalanche
- gate electrode
- 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]
- H10D30/68—Floating-gate IGFETs
- H10D30/681—Floating-gate IGFETs having only two programming levels
- H10D30/684—Floating-gate IGFETs having only two programming levels programmed by hot carrier injection
- H10D30/686—Floating-gate IGFETs having only two programming levels programmed by hot carrier injection using hot carriers produced by avalanche breakdown of PN junctions, e.g. floating gate avalanche injection MOS [FAMOS]
Landscapes
- Semiconductor Memories (AREA)
- Non-Volatile Memory (AREA)
Description
【発明の詳細な説明】
半導体メモリは、蓄えられた情報が電気信号と
して容易かつ高速度で取り出せること、集積回路
(以下ICと称す)技術は発達により大規模集積
(以下LSIと称す)されるようになり、ビツト密
度、信頼性が向上したこと等の理由により、最近
電子計算機の高速用メモリ装置として用いられて
いる。[Detailed Description of the Invention] Semiconductor memory allows stored information to be retrieved easily and at high speed as an electrical signal, and with the development of integrated circuit (hereinafter referred to as IC) technology, large-scale integration (hereinafter referred to as LSI) is possible. Due to its improved bit density and reliability, it has recently been used as a high-speed memory device for electronic computers.
しかしながら半導体メモリは、磁性メモリと異
なり、バイアス電源の供給が断たれると、記憶内
容が消えてしまう(以下揮発性と称す)という欠
点を有していた。この欠点のない半導体メモリを
得べく、従来、例えばカルコゲナイドガラス等の
半導体ガラスの記憶作用についての研究が成され
ているが、未だ実用段階には至つていない。 However, unlike magnetic memories, semiconductor memories have the disadvantage that when the supply of bias power is cut off, the stored contents disappear (hereinafter referred to as volatility). In order to obtain a semiconductor memory that does not have this drawback, research has been carried out on the memory function of semiconductor glasses such as chalcogenide glass, but this has not yet reached a practical stage.
又揮発性のない半導体メモリとして、シリコン
半導体ICの分野に於て、金属(M)・シリコン窒
化膜(N)・シリコン酸化膜(O)・シリコン
(S)の構成を有するMNOS電界効果トランジス
タが開発されたが、この場合、シリコン酸化膜
(SiO2)を半導体表面のキヤリアがトンネルする
程度に薄くしなければならないので、このシリコ
ン酸化膜にピンホール等が生じ易く、しかも記憶
気候がトラツプ準位によるために生産性、再現性
が劣ることとなるおそれがあり、為に電子計算機
には実用化されていない。 In addition, as a non-volatile semiconductor memory, in the field of silicon semiconductor ICs, MNOS field effect transistors having a structure of metal (M), silicon nitride film (N), silicon oxide film (O), and silicon (S) are used. However, in this case, the silicon oxide film (SiO 2 ) must be made thin enough to allow carriers on the semiconductor surface to tunnel, so pinholes are likely to occur in the silicon oxide film, and the memory climate is near trap-like. Because of this, there is a risk that productivity and reproducibility may be degraded due to the position, and for this reason, it has not been put to practical use in electronic computers.
所でこれ以外の半導体メモリの分野として、半
導体メモリの高ビツト密度、高速性を活かして固
定記憶内容を読み出す様になされた読出し専用メ
モリ(以下ROMと称す)がある。このROMの
構成方法には2種類あり、その1つはICを作る
際のホトエツチに用いるガラスマスクに固定情報
をもたせる方法である。他の1つはICを作る際
には記憶すべき内容に関係なく一様に製作し、そ
の後記憶すべき内容に応じて電気的に情報を書き
込む方法である。 However, as another field of semiconductor memory, there is a read-only memory (hereinafter referred to as ROM) which takes advantage of the high bit density and high speed of semiconductor memory to read fixed storage contents. There are two ways to configure this ROM, one of which is to provide fixed information on the glass mask used for photo-etching when making ICs. The other method is to manufacture ICs uniformly regardless of the content to be stored, and then electrically write information in accordance with the content to be stored.
後者の方法は更に3つの方法が知られている。
すなわち、その第1の方法は配線を電流パルスで
溶断する方法であり、第2の方法はアルミナのト
ラツプによる記憶特性を用いる方法であり、第3
の方法はチヤネル電流が流れないときのMOSト
ランジスタのドレインと半導体基板間接合のアバ
ランシエ降服により、半導体基板と同一形のキヤ
リアを酸化膜中に注入し、このキヤリアにより酸
化膜中に埋込まれた多結晶シリコン薄膜層を充電
して情報を書き込む方法である。 Three methods of the latter method are known.
That is, the first method is to fuse the wiring with a current pulse, the second method is to use the memory characteristics of alumina traps, and the third method is
In this method, carriers having the same shape as the semiconductor substrate are injected into the oxide film by avalanche breakdown of the junction between the drain of the MOS transistor and the semiconductor substrate when no channel current flows, and the carriers are buried in the oxide film. This is a method of writing information by charging a polycrystalline silicon thin film layer.
本発明はこれ等3つの方法中の第3の方法に関
連するもので、先ず第1図について、従来の方法
を更に詳述する。この場合、第1図Aに示す如
く、基板1に、その伝導形とは反対の伝導形を有
しかつ不純物濃度の大なるドレイン領域2及びソ
ース領域3と、ゲートシリコン酸化膜4と、シリ
コン酸化膜4及び5間に埋込まれたシリコン多結
晶層6とでなる電界効果トランジスタ7を形成す
る。この電界効果トランジスタ7に於て、ドレイ
ン電圧を増加して行くと、ドレイン領域2から基
板1中に空乏層8が拡がつて行くが、特にシリコ
ン多結晶層6の下の部分9には矢示する如く電界
が集中して空乏層8の他の部分よりも高電界とな
つて行き、遂にはなだれ降服の臨海電界に達す
る。このときこの部分9には第1図Bに示す如く
電子10及び正孔11の電子・正孔対が発生し、
基板1が例えばn形の場合は電界により電子10
が矢12に示す如く酸化膜4の方向へ加速され、
これにより高いエネルギーを得て酸化膜4の中へ
注入される。この様にして注入された電子10は
酸化膜4を通過してシリコン多結晶層6に到達
し、これを負に帯電させる。一方正孔11は電界
によつて矢13の如くドレイン領域2に運ばれ
る。 The present invention relates to the third of these three methods, and the conventional method will first be described in more detail with reference to FIG. In this case, as shown in FIG. 1A, a drain region 2 and a source region 3 having a conductivity type opposite to that of the substrate 1 and having a high impurity concentration, a gate silicon oxide film 4, and a silicon A field effect transistor 7 consisting of a silicon polycrystalline layer 6 buried between oxide films 4 and 5 is formed. In this field effect transistor 7, when the drain voltage is increased, a depletion layer 8 spreads from the drain region 2 into the substrate 1, but especially in the portion 9 below the silicon polycrystalline layer 6, an arrow appears. As shown, the electric field is concentrated and becomes higher than other parts of the depletion layer 8, and finally reaches the critical electric field of avalanche. At this time, electron-hole pairs of electrons 10 and holes 11 are generated in this portion 9, as shown in FIG. 1B.
For example, if the substrate 1 is n-type, the electric field causes electrons 10
is accelerated in the direction of the oxide film 4 as shown by arrow 12,
This obtains high energy and injects it into the oxide film 4. The electrons 10 injected in this manner pass through the oxide film 4 and reach the silicon polycrystalline layer 6, charging it negatively. On the other hand, the holes 11 are transported to the drain region 2 as shown by an arrow 13 by the electric field.
かくしてシリコン多結晶層6の充電状態を得る
ことにより情報の書込みをなし得る。しかしなが
ら上述した従来の方法及び構造では情報の書き込
み、の効率または速度を制御する方法・手段がな
く、書き込み効率または速度を向上させることが
できなかつた。 By thus obtaining the charged state of the silicon polycrystalline layer 6, information can be written. However, in the conventional methods and structures described above, there is no method or means for controlling the efficiency or speed of writing information, and it has not been possible to improve the writing efficiency or speed.
本発明は上述の点を考慮し、情報の書き込みの
効率または速度を向上するなだれ注入型不揮発性
電界効果型トランジスタの書き込み方法を提供す
ることを目的とする。 SUMMARY OF THE INVENTION In view of the above, an object of the present invention is to provide a method for writing an avalanche injection type nonvolatile field effect transistor that improves the efficiency or speed of writing information.
本発明は、一導電型半導体基板に形成され任意
電圧を印加せしめることによつてなだれ降服を発
生する前記一導電型半導体基板と逆導電型のソー
スおよびドレイン領域と、該ソース、ドレイン領
域間の半導体基板上に設けられたゲート絶縁膜
と、前記ゲート絶縁膜に連続した第2の絶縁膜
と、前記ゲート絶縁膜と第2の絶縁膜間に埋込ま
れた第1のゲート電極からなる、なだれ注入型不
揮発性電界効果型トランジスタにおいて、更に前
記第2の絶縁膜を介して第1のゲート電極と対向
する如く設けられた第2のゲート電極を設け、前
記なだれ降服により生成した電荷を前記第1のゲ
ート電極に注入する方向に電位を与えることを特
徴とするなだれ降服注入型不揮発性電界効果トラ
ンジスタの書き込み方法である。 The present invention provides a source and drain region formed on a semiconductor substrate of one conductivity type and having a conductivity type opposite to that of the semiconductor substrate of one conductivity type, which generates avalanche by applying an arbitrary voltage, and a source and drain region between the source and drain regions. consisting of a gate insulating film provided on a semiconductor substrate, a second insulating film continuous with the gate insulating film, and a first gate electrode embedded between the gate insulating film and the second insulating film, In the avalanche injection type nonvolatile field effect transistor, a second gate electrode is provided to face the first gate electrode with the second insulating film interposed therebetween, and the charge generated by the avalanche injection is transferred to the avalanche injection type nonvolatile field effect transistor. This is a writing method for an avalanche injection type nonvolatile field effect transistor characterized by applying a potential in the direction of injection to the first gate electrode.
かかる本発明に依る記憶方法及び記憶装置の特
徴は、以下図面と共に詳述する所により明らかと
なるであろう。 The features of the storage method and storage device according to the present invention will become clearer from the following detailed description in conjunction with the drawings.
先ず第2図について本発明に依る記憶方法につ
いて述べるに、この場合の記憶用電界効果トラン
ジスタ21は、シリコン酸化膜でなる絶縁膜27
上に第2のゲート電極23を設けたことを除いて
は、第1図の電界効果トランジスタ7と同様の構
成を有する。 First, to describe the storage method according to the present invention with reference to FIG. 2, the storage field effect transistor 21 in this case has an insulating film 27 made of a silicon oxide film.
It has the same structure as the field effect transistor 7 of FIG. 1, except that a second gate electrode 23 is provided thereon.
尚、第2図に於て、22はゲート絶縁膜、24
は半導体板、25はドレイン領域、26はソース
領域、27は前記ゲート絶縁膜22に連続する絶
縁膜、28は前記ゲート絶縁膜22及び絶縁膜2
7間に埋込まれた第1のゲート電極、29は空乏
層を夫々示す。 In FIG. 2, 22 is a gate insulating film, and 24 is a gate insulating film.
25 is a drain region, 26 is a source region, 27 is an insulating film continuous to the gate insulating film 22, and 28 is the gate insulating film 22 and the insulating film 2.
The first gate electrode buried between the electrodes 7 and 29 represents a depletion layer, respectively.
所で、電界効果トランジスタ21のゲート絶縁
膜22に基板24中のキヤリアを注入するために
は、キヤリアに対して基板24及び絶縁膜22間
の障壁を越えるに足りるだけのエネルギーを与え
る必要がある。この為第2図の場合は、第2のゲ
ート電極23の電位をたとえば基板24と同電位
とし、ドレイン領域25に基板24との間の降服
電圧以上の電圧を与える。かくすれば、ドレイン
領域25及び基板24間になだれ降服が生じ、こ
れにより電極28及び降服点間の電界に基づき、
電極28の方向に加速されて絶縁膜22中に注入
され、結局電極28に充電されることになる。 By the way, in order to inject the carriers in the substrate 24 into the gate insulating film 22 of the field effect transistor 21, it is necessary to give the carriers enough energy to cross the barrier between the substrate 24 and the insulating film 22. . Therefore, in the case of FIG. 2, the potential of the second gate electrode 23 is set to be the same potential as that of the substrate 24, and a voltage higher than the breakdown voltage with respect to the substrate 24 is applied to the drain region 25. Thus, an avalanche breakdown occurs between the drain region 25 and the substrate 24, which causes the electric field between the electrode 28 and the breakdown point to
It is accelerated in the direction of the electrode 28 and injected into the insulating film 22, and eventually the electrode 28 is charged.
第2図について上述した方法に依れば、情報の
書込みを単に記憶素子としての記憶用電界効果ト
ランジスタのバイアス条件を変更するだけで所望
に応じて確実になし得、しかも一旦書き込まれた
情報は素子に対するバイアスを与えて置かなくと
も、そのまま保存せしめることができる。従つて
この方法による記憶用トランジスタを有する多数
のメモリユニツトセルを実際の装置に組込んだ場
合にも、所望とするビツトを選択して個別に情報
の書込みを極めて容易になし得る。 According to the method described above with reference to FIG. 2, information can be written reliably as desired simply by changing the bias conditions of the storage field effect transistor as a storage element, and once the information has been written, It is possible to preserve the element as it is without applying a bias to the element. Therefore, even when a large number of memory unit cells having storage transistors according to this method are incorporated into an actual device, desired bits can be selected and information can be written individually with great ease.
又この方法を実現する第2図の構成に依れば、
電極23を有するので、電極28に対して注入さ
れたキヤリアを加速せしめる様な電位を与えるこ
とができ、これによりキヤリアの注入速度及び効
率の高い従つて第1のゲート電極28を十分に充
電でき、従つて記憶素子として性能のよい記憶用
電界効果トランジスタを得ることができる。更に
上記の電位を電極28に与えることによりドレイ
ン領域25と基板24との間の降服電圧も第1の
ゲート電極のみの構造にくらべて低下させること
ができるので本構造の素子をアレイ状に接続した
場合の素子選択に用いることもできる。 Also, according to the configuration shown in FIG. 2 that realizes this method,
Since the electrode 23 is provided, a potential that accelerates the injected carriers can be applied to the electrode 28, and thereby the carrier injection speed and efficiency are high, so that the first gate electrode 28 can be sufficiently charged. Therefore, it is possible to obtain a memory field effect transistor with good performance as a memory element. Furthermore, by applying the above potential to the electrode 28, the breakdown voltage between the drain region 25 and the substrate 24 can be lowered compared to the structure with only the first gate electrode, so the elements of this structure can be connected in an array. It can also be used for element selection in such cases.
本発明方法に依る第3図に示す電界効果トラン
ジスタ70を用いて実験した結果、第4図に示す
関係が得られた。この場合、半導体基板24は不
純物濃度5×1013個/cm3のn形シリコンでなり、
ソース領域26の領域46との接合附近の表面不
純物濃度を略々1016個/cm3、ゲート絶縁膜
(SiO2)22の厚さl1を約1000Å、絶縁膜(SiO2)
27の厚さl2を約1000Å、チヤネル長Lを約10μ
mとし、埋込みゲート電極(Si)の電圧が基板2
4に対して「1」書込みの場合0Vから−4V相当
へ、「0」書込みの場合−4Vから0V相当へ夫々
変化するに要する時間を測定し、その結果を第2
のゲート電極23(Al)及びソース領域26
(P)の端子電圧VGSに対する時間tとして表し
たものである。 As a result of an experiment using the field effect transistor 70 shown in FIG. 3 according to the method of the present invention, the relationship shown in FIG. 4 was obtained. In this case, the semiconductor substrate 24 is made of n-type silicon with an impurity concentration of 5×10 13 /cm 3 ,
The surface impurity concentration near the junction of the source region 26 with the region 46 is approximately 10 16 /cm 3 , the thickness l 1 of the gate insulating film (SiO 2 ) 22 is approximately 1000 Å, and the insulating film (SiO 2 )
The thickness l 2 of 27 is approximately 1000 Å, and the channel length L is approximately 10 μ.
m, and the voltage of the buried gate electrode (Si) is
For 4, measure the time required to change from 0V to -4V equivalent when writing "1", and from -4V to 0V equivalent when writing "0", and compare the results to the second
gate electrode 23 (Al) and source region 26
It is expressed as time t versus terminal voltage VGS of (P).
尚第4図に於て、符号は、ドレイン端子D及
びソース端子Sを接地し、基板端子Bに正バイア
スを与え、ソース領域26及び領域46間接合の
逆方向電流を100μAとした場合に得られた曲線
を、符号は基板端子Bを接地し、ドレイン端子
Dに負バイアスを与え、ソース端子Sに少し負バ
イアスを与え、基板24及びドレイン領域25間
接合の逆方向電流を10μAとした場合に得られた
曲線を、夫々示す。尚、符号で示す曲線がドレ
イン基板間になだれ降服を生起させた本発明の実
施例である。 In FIG. 4, the symbols indicate the values obtained when the drain terminal D and source terminal S are grounded, the substrate terminal B is given a positive bias, and the reverse current in the junction between the source region 26 and the region 46 is 100 μA. The sign of the curve is when the substrate terminal B is grounded, the drain terminal D is given a negative bias, the source terminal S is given a slight negative bias, and the reverse current at the junction between the substrate 24 and the drain region 25 is 10 μA. The curves obtained are shown respectively. Note that the curve indicated by the symbol is an example of the present invention in which avalanche precipitation occurred between the drain substrate.
この測定結果から、第1に第2ゲート電極23
を設けることによつて書込み時間を格段的に高速
化し得ること、第2に第2のゲート電極23の電
圧が電子の注入を促す方向に変化したとき著しく
書込み時間が短縮されること、すなわち第2ゲー
ト電圧でなだれ降服で生成した電荷を第1のゲー
ト電極へ注入する方向を与えること、第3に書込
み時間は降服を起こしている接合のなだれ降服電
流に反比例して小さくなることが実証された。更
に第2ゲート電極のバイアスにより書き込まれる
トランジスタをアレイ状に配置されたセルから選
択できることもわかつた。 From this measurement result, firstly, the second gate electrode 23
Second, when the voltage of the second gate electrode 23 changes in a direction that promotes electron injection, the writing time is significantly shortened. It has been demonstrated that two gate voltages direct the charge generated by avalanche breakdown into the first gate electrode, and third, the writing time decreases inversely with the avalanche current of the junction undergoing breakdown. Ta. Furthermore, it has been found that the transistor to be written can be selected from the cells arranged in an array by biasing the second gate electrode.
上述の如く本発明に依れば、半導体メモリが本
来有している読出しの高速性と、従来磁気メモリ
によつてしか実用化されていなかつた記憶の不揮
発性とを兼ね備えた半導体メモリを得ることがで
き、かかるメモリを製作するにつき、従来のシリ
コンゲート技術又はモリブデンゲート技術を用
い、他に何等特殊な技術を要することなく、容易
に高密度に製作することができるものである。 As described above, according to the present invention, it is possible to obtain a semiconductor memory that combines the high speed of readout that semiconductor memory inherently has and the nonvolatile memory that has conventionally been put into practical use only with magnetic memory. When manufacturing such a memory, it is possible to easily manufacture it at high density using conventional silicon gate technology or molybdenum gate technology without requiring any other special technology.
また、本発明の依れば、記憶用不揮発性電界効
果トランジスタと書込み時の印加電圧を必要十分
に設定できるので、記憶用不揮発性電界効果トラ
ンジスタの書込み動作を確実にし、しかも高速化
が可能であり、安定な動作をはかることができる
利点を有する。 Further, according to the present invention, since the voltage applied to the memory non-volatile field effect transistor and the voltage applied during writing can be set to the necessary and sufficient level, the write operation of the memory non-volatile field effect transistor can be ensured and can be made faster. It has the advantage of stable operation.
尚、以上の説明では記憶内容が「1」と「0」
のデイジタル情報であつたが不揮発性アナログ情
報の記憶に用いることもできることは明らかであ
る。又、本発明のトランジスタに蓄積された情報
は紫外線で消去できる。 In addition, in the above explanation, the memory contents are "1" and "0".
It is clear that it can also be used to store non-volatile analog information, although this is digital information. Furthermore, the information stored in the transistor of the present invention can be erased with ultraviolet light.
第1図は従来の情報書込方法の説明に供する電
界効果トランジスタを示す断面図、第2図は本発
明に依る不揮発性メモリの記憶方法の一例の説明
に供する記憶用電界効果トランジスタを示す断面
図、第3図及び第4図は本発明方法の一例による
実験結果を示す図である。
図中、21,70……記憶用電界効果トランジ
スタ、22……ゲート絶縁膜、23……第2のゲ
ート電極、24……半導体基板、25……ドレイ
ン領域、26,54……ソース領域、27……絶
縁膜、28……第1のゲート電極、29……空乏
層、30……チヤネル、31……ピンチオフ領
域。
FIG. 1 is a sectional view showing a field effect transistor for explaining a conventional information writing method, and FIG. 2 is a cross section showing a storage field effect transistor for explaining an example of a nonvolatile memory storage method according to the present invention. 3 and 4 are diagrams showing experimental results according to an example of the method of the present invention. In the figure, 21, 70... memory field effect transistor, 22... gate insulating film, 23... second gate electrode, 24... semiconductor substrate, 25... drain region, 26, 54... source region, 27... Insulating film, 28... First gate electrode, 29... Depletion layer, 30... Channel, 31... Pinch-off region.
Claims (1)
基板に形成され任意電圧を印加せしめることによ
つてなだれ降服を発生する前記一導電型半導体基
板と逆導電型のドレイン領域と、逆導電型のソー
ス領域と、該ソース、ドレイン領域間の半導体基
板上に設けられたゲート絶縁膜と、前記ゲート絶
縁膜に連続した第2の絶縁膜と、前記ゲート絶縁
膜と第2の絶縁膜に埋込まれた第1のゲート電極
からなる、なだれ注入型不揮発性電界効果型トラ
ンジスタにおいて、更に前記第2の絶縁膜を介し
て第1のゲート電極と対向する如く設けられた第
2のゲート電極を設け、前記なだれ降服によつて
生成した電荷を前記第1のゲート電極に注入する
方向に電位を与えることを特徴とするなだれ降服
注入型不揮発性電界効果トランジスタの書き込み
方法。1 A semiconductor substrate of one conductivity type, a drain region of the opposite conductivity type to the one conductivity type semiconductor substrate, which is formed on the one conductivity type semiconductor substrate and generates avalanche precipitation by applying an arbitrary voltage, and a drain region of the opposite conductivity type. a source region, a gate insulating film provided on a semiconductor substrate between the source and drain regions, a second insulating film continuous with the gate insulating film, and a second insulating film embedded in the gate insulating film and the second insulating film. In the avalanche injection type nonvolatile field effect transistor, the avalanche injection type nonvolatile field effect transistor is further provided with a second gate electrode provided so as to face the first gate electrode with the second insulating film interposed therebetween. . A writing method for an avalanche injection nonvolatile field effect transistor, characterized in that a potential is applied in a direction to inject charges generated by the avalanche into the first gate electrode.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57046705A JPS57167682A (en) | 1982-03-24 | 1982-03-24 | Avalanche breakdown injection type field-effect transistor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57046705A JPS57167682A (en) | 1982-03-24 | 1982-03-24 | Avalanche breakdown injection type field-effect transistor |
Related Parent Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP55026400A Division JPS5833713B2 (en) | 1980-03-03 | 1980-03-03 | Non-volatile memory unit cell |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57167682A JPS57167682A (en) | 1982-10-15 |
| JPH0353788B2 true JPH0353788B2 (en) | 1991-08-16 |
Family
ID=12754775
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57046705A Granted JPS57167682A (en) | 1982-03-24 | 1982-03-24 | Avalanche breakdown injection type field-effect transistor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57167682A (en) |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5510151A (en) * | 1978-07-07 | 1980-01-24 | Honda Motor Co Ltd | Power transmitting apparatus |
| JPS5537107A (en) * | 1978-09-05 | 1980-03-15 | Iseki Agricult Mach | Separator of thresher |
-
1982
- 1982-03-24 JP JP57046705A patent/JPS57167682A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57167682A (en) | 1982-10-15 |
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