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JPH0585990B2 - - Google Patents
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JPH0585990B2 - - Google Patents

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Publication number
JPH0585990B2
JPH0585990B2 JP59067221A JP6722184A JPH0585990B2 JP H0585990 B2 JPH0585990 B2 JP H0585990B2 JP 59067221 A JP59067221 A JP 59067221A JP 6722184 A JP6722184 A JP 6722184A JP H0585990 B2 JPH0585990 B2 JP H0585990B2
Authority
JP
Japan
Prior art keywords
voltage
potential
vcc
electrode
transistor
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 - Fee Related
Application number
JP59067221A
Other languages
Japanese (ja)
Other versions
JPS60211689A (en
Inventor
Yoshihiro Takemae
Tomio Nakano
Kimiaki Sato
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP59067221A priority Critical patent/JPS60211689A/en
Publication of JPS60211689A publication Critical patent/JPS60211689A/en
Publication of JPH0585990B2 publication Critical patent/JPH0585990B2/ja
Granted legal-status Critical Current

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Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11CSTATIC STORES
    • G11C11/00Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor
    • G11C11/21Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor using electric elements
    • G11C11/34Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor using electric elements using semiconductor devices

Landscapes

  • Engineering & Computer Science (AREA)
  • Computer Hardware Design (AREA)
  • Semiconductor Memories (AREA)

Description

【発明の詳細な説明】 発明の技術分野 本発明は、1トランジスタ1キヤパシタ型のメ
モリセルを備えそのキヤパシタの対向電極を電源
電圧と接地電位の中間電位とするダイナミツク型
半導体記憶装置に関する。
TECHNICAL FIELD OF THE INVENTION The present invention relates to a dynamic type semiconductor memory device that includes a one-transistor, one-capacitor type memory cell, and has a counter electrode of the capacitor at an intermediate potential between a power supply voltage and a ground potential.

従来技術と問題点 ダイナミツク型半導体記憶装置のメモリセルは
一般に1トランジスタ1キヤパシタ型であり、該
キヤパシタは半導体基板表面の絶縁膜を誘導体、
該絶縁膜上のメタルまたは多結晶シリコンを一方
の電極、その下部の半導体基板を他方の電極とし
てするMOS型として構成され、特に該一方の電
極(対向電極という)に電源電圧+Vccを加えて
その下部のp型半導体基板をn反転させこれを他
方の電極とするものが広く用いられる。また対向
電極に加える電圧はVccでなくてもよく、基板に
n型不純物を拡散させてn型化すれば対向電極電
位は電源電圧Vccと接地電位0ボルトの中間電位
でも或いは接地電位そのものでもよい。
Prior Art and Problems The memory cell of a dynamic semiconductor memory device is generally of the one-transistor, one-capacitor type, and the capacitor is formed by using a dielectric film or a dielectric film on the surface of the semiconductor substrate.
It is configured as a MOS type in which the metal or polycrystalline silicon on the insulating film is used as one electrode, and the semiconductor substrate below it is used as the other electrode. A device in which the lower p-type semiconductor substrate is n-inverted and used as the other electrode is widely used. Also, the voltage applied to the counter electrode does not have to be Vcc; if the substrate is made n-type by diffusing n-type impurities, the counter electrode potential can be an intermediate potential between the power supply voltage Vcc and the ground potential of 0 volts, or the ground potential itself. .

メモリは益々大容量化され、つれてメモリセル
は益々小型化される傾向にある。小型化には各部
均等縮尺が必要であり、つれて絶縁膜なども薄く
する必要があり、耐圧の点で問題がでてくる。即
ちキヤパシタの対向電極にVccを加え、他方の電
極つまり半導体基板にVccで電荷を蓄え又は蓄え
ない(データ“1”、“0”を記憶させる)と、該
他方の電極の電位はVcc又はVss(0ボルト)で
あるから、キヤパシタの絶縁膜には最高でVccが
加わる。これは、膜厚が薄いと強い電界を生じ、
絶縁膜は絶縁破壊する恐れがある。そこで対向電
極には中間電位例えばVcc/2を加えることが考
えられている。これなら、他方の電極がVcc,
Vssのいずれでも対向電極との電位差はVcc/2
で、上記の半分になり、絶縁破壊の問題は大幅に
軽減される。かゝるダイナミツクメモリの要部を
第1図に示す。
As memories become larger and larger, memory cells tend to become smaller and smaller. Miniaturization requires uniform scaling of all parts, and as a result, insulating films and the like must also be made thinner, which poses problems in terms of withstand voltage. That is, when Vcc is applied to the opposing electrode of the capacitor, and the other electrode, that is, the semiconductor substrate, stores or does not store charge at Vcc (data "1" and "0" are stored), the potential of the other electrode becomes Vcc or Vss. (0 volt), Vcc is applied to the capacitor's insulating film at most. This produces a strong electric field when the film is thin,
There is a risk of dielectric breakdown of the insulating film. Therefore, it has been considered to apply an intermediate potential, for example, Vcc/2, to the counter electrode. In this case, the other electrode is Vcc,
For either Vss, the potential difference with the counter electrode is Vcc/2
This is half of the above value, and the problem of dielectric breakdown is greatly reduced. The main parts of such a dynamic memory are shown in FIG.

第1図で、WLはワード線、BL,はビツト
線対、SAはセンスアンプMCはMOSトランジス
タQ1およびキヤパシタC1からなるメモリセルで
ある。分圧回路VDは抵抗値の等しい2つの抵抗
R1,R2をVccとVss間に直列に接続してなり、こ
の中間接続点がセル対向電極OPに接続される。
対向電極OPは多数のメモリセルに共通であり、
図ではワード線と同様な配線の形で示している。
Eは他方の電極であり、これはトランジスタQ1
のソースと一体化されることもある。この他方の
電極EとトランジスタQ1のソースとの接続部を
ノードN1で示す。
In FIG. 1, WL is a word line, BL is a bit line pair, and SA is a sense amplifier MC, which is a memory cell consisting of a MOS transistor Q1 and a capacitor C1 . Voltage divider circuit VD consists of two resistors with equal resistance value.
R 1 and R 2 are connected in series between Vcc and Vss, and this intermediate connection point is connected to the cell counter electrode OP.
The counter electrode OP is common to many memory cells,
In the figure, it is shown in a wiring form similar to a word line.
E is the other electrode, which is the transistor Q 1
Sometimes it is integrated with the source. The connection between this other electrode E and the source of the transistor Q1 is indicated by a node N1 .

ところで対向電極OPは大面積であり、ビツト
線BL,などと交叉してそれらとの間に大きな
浮遊容量Cp1,Cp2等を持つ結果、それらの信号線
の電位変化に伴い容量結合によつて電位変動を生
じる。そこで対向電極OPの電位を常に正しく
Vcc/2に保つにはこれらの浮遊容量と分圧回路
VD内の抵抗との時定数が問題となる。勿論、こ
の時定数は小さいほど良い。しかし、抵抗R1
R2に流れる電流はメモリチツプに電源が投入さ
れている限り流れる電流であるから、R1,R2
小さくすると常時消費電力が増大する。従つて抵
抗R1,R2は高抵抗にして消費電力の増大を避け
ねばならない。しかし抵抗R1,R2の値が大きく、
対向電極OPの充放電が即座にはできない状態で
あると、前記寄生容量によるビツト線等との結合
で対向電位は変動する。この変動の詳細は可成り
複雑であるが、概述すれば次の如くである。即
ち、メモリは、センスアンプSAが動作してビツ
ト線BL,の一方をH(ハイ)レベルまたは
Vcc、他方をL(ロー)レベル即ちVssにしたア
クテイブな状態と、センスアンプSAは動作せず
ビツト線BL,がHレベルVccにチヤージされ
たスタンバイ状態をとるが、上記分圧回路による
充放電を時定数大故に無視すると、対向電極OP
は前者つまりアクテイブのときは後者スタンバイ
のときよりも寄生容量Cp1又はCp2の一方での容量
結合による変動分だけ低い電位をとる。
By the way, the counter electrode OP has a large area and intersects with the bit line BL, etc., and has large stray capacitances C p1 , C p2 , etc. between them, and as a result, capacitive coupling occurs due to changes in the potential of those signal lines. As a result, potential fluctuations occur. Therefore, the potential of the counter electrode OP must always be adjusted correctly.
To maintain Vcc/2, these stray capacitances and voltage divider circuits are required.
The time constant with the resistance in VD becomes a problem. Of course, the smaller this time constant is, the better. However, the resistance R 1 ,
Since the current flowing through R 2 continues to flow as long as the power is applied to the memory chip, reducing R 1 and R 2 constantly increases power consumption. Therefore, resistors R 1 and R 2 must have high resistance to avoid an increase in power consumption. However, the values of resistance R 1 and R 2 are large,
If the counter electrode OP cannot be charged or discharged immediately, the counter potential will fluctuate due to coupling with the bit line etc. due to the parasitic capacitance. Although the details of this variation are quite complicated, they can be summarized as follows. That is, in the memory, the sense amplifier SA operates to set one of the bit lines BL to H (high) level or
There is an active state in which Vcc and the other are set to L (low) level, that is, Vss, and a standby state in which the sense amplifier SA does not operate and the bit line BL is charged to the H level, Vcc. is ignored due to the time constant, the counter electrode OP
When the former is active, the potential is lower than when the latter is standby by the amount of variation due to capacitive coupling of one of the parasitic capacitances C p1 and C p2 .

アクテイブ、スタンバイが繰り返されると対向
電極電位は上記2値の間を変動するが、実際には
これに寄生容量の充放電による影響が加わる。即
ちOP=Vcc/2ならCp2にはOP側を+、側を
−とする極性で電荷が充電され該極性の電圧
Vcc/2を持つ。この状態で=Vccにすると
Cp2の電圧によりOPは突き上げられ、同時に寄生
容量Cp1,Cp2では電荷の充放電が行なわれる。突
き上げられたOPの電位をVcc/2+ΔVHとすると、 Cp1,Cp2の電圧はVcc/2−ΔVH、Cp2の充電電荷の 極性は前と逆になる。この状態でが再びVss
になると、OPはCp2により押し下げられ、同時に
寄生容量Cp1,Cp2の充放電が行なわれる。この押
し下げられたOPの電位をVcc/2−ΔVLとすると、 Cp1の電圧はVcc/2+ΔVL,Cp2の電圧はVcc/2− ΔVLで極性は最初の状態に戻る。スタンバイ期間
とアクテイブ期間が同じ長さの場合はΔVHはΔVL
に等しい。
When active and standby are repeated, the counter electrode potential fluctuates between the above two values, but in reality, this is affected by charging and discharging of parasitic capacitance. In other words, if OP = Vcc/2, C p2 is charged with a polarity with the OP side being + and the OP side being -, and the voltage of that polarity is
It has Vcc/2. In this state, if = Vcc
OP is pushed up by the voltage of C p2 , and at the same time charges are charged and discharged in the parasitic capacitances C p1 and C p2 . If the potential of the pushed-up OP is Vcc/2+ΔV H , the voltages of C p1 and C p2 are Vcc/2−ΔV H , and the polarity of the charged charge of C p2 is opposite to that before. In this state, Vss is again
When this happens, OP is pushed down by C p2 and at the same time the parasitic capacitances C p1 and C p2 are charged and discharged. If the potential of this pushed down OP is Vcc/2-ΔV L , the voltage of C p1 is Vcc/2+ΔV L , the voltage of C p2 is Vcc/2-ΔV L , and the polarity returns to the initial state. If the standby period and active period are the same length, ΔV H is ΔV L
be equivalent to.

こうして対向電極OPの電位はVcc/2+ΔVHと Vcc/2−ΔVLとの間を変化するが、これはアクテ イブ、スタンバイが短時間で繰り返されている場
合であつて、アクテイブ期間またはスタンバイ期
間が長くなると、OPは分圧回路VDによりVcc/
2を与えられるのでこのVcc/2へ落ち付くこと
になる。Vcc/2へ落ち付いた状態で、例えば今
までスタンバイであつたものがアクテイブにな
り、BL=H,=Lになると、Cp2による押し
下げが生じ、OPの電位はVcc/2−(ΔVL+ΔVH) にもなる。なお前記説明ではこれはVcc/2−ΔVL としたが、それは前の状態がVcc/2+ΔVHにあつ たからであり、変動幅は同じΔVL+ΔVHである。
今までアクテイブであつたものがスタンバイに変
つたときも同様で、この場合はVcc/2+ΔVH+ ΔVLへ突き上げられる。
In this way, the potential of the counter electrode OP changes between Vcc/2 + ΔV H and Vcc/2 - ΔV L , but this is a case where active and standby are repeated in a short time, and the active period or standby period is When the length becomes longer, OP becomes Vcc/
2 is given, so it will settle down to this Vcc/2. When the voltage has settled down to Vcc/2, for example, what had been on standby becomes active and BL = H, = L, a depression occurs due to C p2 , and the potential of OP becomes Vcc/2 - (ΔV L +ΔV H ). In the above description, this is set to be Vcc/2-ΔV L , but this is because the previous state was Vcc/2+ΔV H , and the fluctuation range is the same, ΔV L +ΔV H.
The same thing happens when what has been active until now changes to standby; in this case, it is pushed up to Vcc/2 + ΔV H + ΔV L.

このようなOPの電位の変動は、アクテイブ期
間とスタンバイ期間との比率が比較的長時間にわ
たつて変化した場合にも同様に生じる。前述のよ
うに対向電極に中間電位Vcc/2を与えるのは絶
縁膜の絶縁劣化を防ぐためであるが、その対向電
極の電位が上記のように大幅に変つてしまうので
は中間電位採用の効果が減殺されてしまう。また
対向電極OPの電位は他方の電極E、従つてノー
ドN1の電位に影響し、OPの電位が大きく下ると
N1の電位も大きく下つてセンスアンプSAが誤動
作し、データ“1”記憶状態もデータ“0”記憶
状態と誤判定される恐れがある。
Such fluctuations in the potential of OP similarly occur when the ratio between the active period and the standby period changes over a relatively long period of time. As mentioned above, applying the intermediate potential Vcc/2 to the counter electrode is to prevent insulation deterioration of the insulating film, but if the potential of the counter electrode changes significantly as described above, the effect of adopting the intermediate potential is poor. will be reduced. Also, the potential of the opposing electrode OP affects the potential of the other electrode E, and hence the node N1 , and if the potential of the OP drops significantly,
The potential of N1 also drops significantly, causing the sense amplifier SA to malfunction, and the data "1" storage state may be erroneously determined to be the data "0" storage state.

そこで本発明者は分圧回路VDの出力をアクテ
イブ時とスタンバイ時で切換えることを考え、こ
れを先に提案した(特願昭57−211146号)。第1
図の抵抗R3,MOSトランジスタQ2がこれで、ク
ロツクφAによりトランジスタQ2をオンオフする
ことにより分圧回路の出力レベルをH,Lに変え
る。即ちクロツクφAはアクテイブ時にH、スタ
ンバイ時にLとすると、アクテイブ時にはトラン
ジスタQ2がオンになつて抵抗R2に抵抗R3を並列
接続し、分圧回路の出力を下げ、スタンバイ時に
はトランジスタQ2をオフにして抵抗R3を切り離
し、分圧回路の出力を上げる。OPの平均電位を
Vcc/2とするにはR1,R2の抵抗値は異ならせ
る。つまり分圧回路VDのHレベル出力は前記の
Vcc/2+ΔVH,Lレベル出力はVcc/2−ΔVLに選ぶ と、アクテイブ期間及びスタンバイ期間が長くな
つても、対向電極電位の落ち付き先と分圧回路の
出力レベルが同じであるから変化がなく、アクテ
イブ、スタンバイの再開で対向電極電位が大きく
変動することがない。
Therefore, the inventor of the present invention considered switching the output of the voltage divider circuit VD between active and standby states, and previously proposed this (Japanese Patent Application No. 57-211146). 1st
The resistor R 3 and MOS transistor Q 2 shown in the figure turn on and off the transistor Q 2 using the clock φ A , thereby changing the output level of the voltage dividing circuit between H and L. That is, if the clock φ A is set to H during active and L during standby, transistor Q 2 turns on during active, connects resistor R 2 and resistor R 3 in parallel, and lowers the output of the voltage divider circuit, and during standby, transistor Q 2 turns on. Turn off to disconnect resistor R3 and increase the output of the voltage divider circuit. The average potential of OP is
To set it to Vcc/2, the resistance values of R 1 and R 2 are made different. In other words, the H level output of the voltage divider circuit VD is
Vcc/2+ΔV H , L level output is selected to be Vcc/2−ΔV L , even if the active period and standby period are long, the potential settling of the counter electrode and the output level of the voltage divider circuit are the same, so there is no change. There is no significant fluctuation in the potential of the counter electrode when active or standby is restarted.

しかしながらこの既提案回路にも欠点がある。
即ち、前述のように消費電力を少なくするため、
抵抗R1,R2は高抵抗であり、つれて抵抗R3も高
抵抗であるが、高抵抗であると寄生容量などと大
きな時定数を作つてしまう。特に抵抗R3の挿脱
のためMOSトランジスタQ2を用いると、これは
大きなソース、ドレイン容量を持つており、この
ためトランジスタQ2をオフにしても直ちにはノ
ードN2の電位が上らず、抵抗R3が接続されてい
るのと同じ状態になつてしまう。第2図はこれを
説明する図で、曲線N2はノードN2の電位変化を
示す。同様に曲線φAはクロツクφA、曲線OPは対
向電極OPの電位変化を示す。はローアドレ
スストローブ信号で、外部より与えられ、Lレベ
ルでメモリチツプのセンスアンプSAはアクテイ
ブ、Hレベルでスタンバイになる。前述のように
アクテイブになるとビツト線BL,は一方が
H、他方がLになり、対向電極OPの電位は下り、
スタンバイになるとビツト線BL,は共にHに
なり対向電極の電位が上る。この対向電極OPの
電位変化に合わせてクロツクφAをH,Lにし、
分圧回路VDの出力レベルを変える。即ちアクテ
イブでφAをHにしてトランジスタQ2をオンにし、
ノードN2をVssへ落とし、抵抗R3をR2に並列に
接続する。これは直ちに行なえるので、分圧回路
の出力は急速にLレベルになる。しかしスタンバ
イでクロツクφAをLにし、トランジスタQ2をオ
フにしても、図示のようにノードN2の電位は
中々上らない。ノードN2の電位を上げるには高
抵抗R1,R3を通して該ノードを充電する必要が
あるが、これには時間がかゝる。ノードN2の電
位が上らないとこれは抵抗R3を抵抗R2に並列接
続しているのと同じで分圧回路VDの出力はLレ
ベルである。この状態ではOPの電位は低く、
Cp1,Cp2はBL,側を+にして高い電圧に充電
され、この状態でアクテイブになつて例えば
がVssになるとOPは強く押し下げられ、キヤパ
シタ絶縁膜の劣化、記憶データの読み誤りを生じ
る恐れがある。
However, this proposed circuit also has drawbacks.
That is, in order to reduce power consumption as mentioned above,
Resistors R 1 and R 2 have high resistance, and resistor R 3 also has high resistance, but high resistance creates parasitic capacitance and a large time constant. In particular, when MOS transistor Q 2 is used to insert and remove resistor R 3 , it has large source and drain capacitances, so even if transistor Q 2 is turned off, the potential at node N 2 does not rise immediately. , the state will be the same as if the resistor R 3 was connected. FIG. 2 is a diagram for explaining this, and a curve N 2 shows a change in the potential of the node N 2 . Similarly, the curve φ A shows the potential change of the clock φ A and the curve OP shows the potential change of the counter electrode OP. is a row address strobe signal, which is applied from the outside.When it is at L level, the sense amplifier SA of the memory chip is active, and when it is at H level, it is in standby. As mentioned above, when the bit line BL becomes active, one becomes H and the other becomes L, and the potential of the counter electrode OP decreases.
When in standby, both bit lines BL and BL become H, and the potential of the opposing electrode rises. The clock φ A is set to H and L in accordance with the potential change of the counter electrode OP,
Change the output level of the voltage divider circuit VD. That is, in the active state, φ A is set to H and transistor Q 2 is turned on.
Drop node N 2 to Vss and connect resistor R 3 in parallel with R 2 . Since this can be done immediately, the output of the voltage divider circuit quickly becomes L level. However, even if the clock φ A is set to L during standby and the transistor Q 2 is turned off, the potential of the node N 2 does not rise as shown in the figure. In order to raise the potential of node N2 , it is necessary to charge the node through high resistances R1 and R3 , but this takes time. If the potential of node N2 does not rise, this is the same as connecting resistor R3 to resistor R2 in parallel, and the output of voltage divider circuit VD is at L level. In this state, the potential of OP is low,
C p1 and C p2 are charged to a high voltage with the BL side set to +, and when they become active in this state and, for example, become Vss, OP is strongly pushed down, causing deterioration of the capacitor insulating film and misreading of stored data. There is a fear.

発明の目的 本発明はかゝる点を改善し、対向電極に与える
中間電位をH,Lに迅速に切換え可能にしようと
するものである。
OBJECTS OF THE INVENTION The present invention aims to improve the above points and to make it possible to quickly switch the intermediate potential applied to the counter electrode between H and L.

発明の構成 本発明は、トランジスタと、該トランジスタに
一方の電極が接続されたキヤパシタよりなる1ト
ランジスタ1キヤパシタ型ダイナミツク・メモリ
セルを備え、前記キヤパシタの他方の電極には電
源電圧よりも低い電圧が与えられる半導体記憶装
置に於いて、前記電源電圧の略中間電圧よりも所
定値だけ高い第1電圧と、前記略中間電圧よりも
所定値だけ低い第2電圧を同時に出力可能な電圧
発生回路と、スタンバイ時には前記第1電圧を、
アクテイブ時には前記第2電圧を、選択的に切り
換えて前記キヤパシタの他方の電極へ供給するス
イツチング素子とを具備することを特徴とする
が、次に実施例を参照しながらこれを説明する。
Structure of the Invention The present invention includes a one-transistor, one-capacitor type dynamic memory cell consisting of a transistor and a capacitor having one electrode connected to the transistor, and the other electrode of the capacitor has a voltage lower than the power supply voltage. In the given semiconductor memory device, a voltage generating circuit capable of simultaneously outputting a first voltage higher than a substantially intermediate voltage of the power supply voltage by a predetermined value and a second voltage lower than the substantially intermediate voltage by a predetermined value; During standby, the first voltage is
The device is characterized by comprising a switching element that selectively switches and supplies the second voltage to the other electrode of the capacitor when it is active, which will be explained next with reference to embodiments.

発明の実施例 第3図は本発明の実施例を示し、第1図と同じ
部分には同じ符号が付してある。本発明では高抵
抗分圧回路はHレベル出力とLレベル出力を生じ
る2端子を備え、対向電極OPはこれらの2端子
の一方へスイツチングトランジスタQ3,Q4で選
択して接続する。抵抗R1とR2がそのHレベル出
力用回路、抵抗R4とR3がLレベル出力用回路で
あり、N3,N4がその出力端である。クロツクφA
がHレベルのときトランジスタQ4がオンになり
対向電極OPへLレベル出力OLを加える。またク
ロツクφAと逆相のクロツクAがHレベルのとき
トランジスタQ3がオンになり、対向電極OPへH
レベル出力OHを加える。前述のように出力OH
1/2Vcc+ΔVHに、また出力OLは1/2Vcc−ΔVLに 選ぶ、即ちメモリがアクテイブ、スタンバイを繰
り返しているときの対向電極OPのH,L2種の電
位に選ぶ。このようにすれば、アクテイブ、スタ
ンバイ期間が長くなつても、対向電極電位に変化
がない。この分圧回路はその出力端N3,N4に常
時、H,L2種の電圧を生じており、その一方を
スイツチング素子Q3,Q4で選択して対向電極OP
へ加えるだけであるから、該電圧印加は直ちに行
なわれ、第1図の回路のように時定数により煩わ
されて直ちには所望電位にならないという問題は
ない。
Embodiment of the Invention FIG. 3 shows an embodiment of the invention, in which the same parts as in FIG. 1 are given the same reference numerals. In the present invention, the high resistance voltage divider circuit has two terminals that produce an H level output and an L level output, and the opposing electrode OP is selectively connected to one of these two terminals by switching transistors Q 3 and Q 4 . Resistors R 1 and R 2 are the H level output circuit, resistors R 4 and R 3 are the L level output circuit, and N 3 and N 4 are the output ends thereof. Clock φ A
When is at H level, transistor Q4 is turned on and applies L level output O L to the opposite electrode OP. Also, when clock A , which has the opposite phase to clock φA , is at H level, transistor Q3 is turned on, and the opposite electrode OP is connected to H level.
Add level output O H. As mentioned above, the output O H is selected to be 1/2Vcc + ΔV H , and the output O L is selected to be 1/2Vcc - ΔV L , that is, the potentials of the H and L types of the opposing electrode OP when the memory is repeatedly active and standby. choose. In this way, even if the active and standby periods become longer, there is no change in the potential of the counter electrode. This voltage divider circuit always generates two voltages, H and L, at its output terminals N 3 and N 4 , and one of them is selected by switching elements Q 3 and Q 4 and the opposite electrode is OP.
Since the voltage application is performed immediately, there is no problem that the desired potential cannot be reached immediately due to a time constant as in the circuit shown in FIG.

第4図は第2図と同様な図であるが、第4図で
はクロツクφAの他にクロツクAも示している。
RASは図示していないが、やはりがLレベ
ルになつて対向電極OPの電位が下り、がH
になつて対向電極OPの電位が上る。クロツクφA
はOPが下つてから立ち上げ、OPが上る前に立ち
下げる。同様にクロツクAはOPが上つてから立
ち上げ、OPが下る前に立ち下げる。OPの電位変
化中はφAAいずれもLであり、トランジスタ
Q3,Q4はオフで対向電極OPはフローテイングの
状態にある。
FIG. 4 is a diagram similar to FIG. 2, but in addition to the clock φA , a clock A is also shown in FIG.
Although RAS is not shown, it also goes to L level, the potential of the counter electrode OP decreases, and RAS goes to H level.
As the voltage increases, the potential of the counter electrode OP increases. Clock φ A
Start up after OP goes down, and down before OP goes up. Similarly, clock A starts up after OP goes up, and goes down before OP goes down. During the potential change of OP, both φ A and A are L, and the transistor
Q 3 and Q 4 are off and the counter electrode OP is in a floating state.

対向電極OPの電位変化中は該OPを分圧回路か
ら切り離す理由は次の如くである。即ちが
Lになつてセンスアンプが動作しOPの電位が下
るが、この電位変化は急激ではない。そこでOP
が十分1/2Vcc−ΔVLの即ちOLの電位Lに達し
ないうちにφAを上げQ4をONとするとわずかの時
間であるがOPよりQ4,N4,R3を通してVssに電
流が流出する。R3の抵抗も高いため1回の流出
量はわずかであるが、数多くこのような現象が繰
返されると、OPの電位は低下する。またφAの立
ち下がり時もOPが立ち上がる前にφAを下げQ4
完全にOFFとしておかないと同様な問題が生ず
る。この問題はAについても同様である。そし
てOP電位の立下り時と立上り時とで電流の流出
量が相違することによつてアクテイブ、スタンバ
イを繰返すうちに、該繰返し周期に依存した且つ
H,Lと異なる電位にOPの電位が変化して行く
ことになる。これを避けるためには第4図に示す
ごとく、OPの電位が完全にOL又はOHの時のみφ4
又はφ3をONとして、OPの電位変化時Q4,Q3
にOFFとする事で可能である。
The reason why the counter electrode OP is separated from the voltage dividing circuit while the potential of the counter electrode OP is changing is as follows. That is, the voltage becomes L, the sense amplifier operates, and the potential of OP drops, but this potential change is not rapid. So OP
If φ A is raised and Q 4 is turned on before it reaches 1/2 Vcc - ΔV L , that is, the potential L of O L , the current will flow from OP to Vss through Q 4 , N 4 , and R 3 for a short time. flows out. Since the resistance of R 3 is also high, the amount of leakage at one time is small, but if this phenomenon is repeated many times, the potential of OP will decrease. Also, when φA falls, a similar problem will occur unless φA is lowered and Q4 is completely turned off before OP rises. This problem also applies to A. As the amount of current flowing out is different when the OP potential falls and rises, as the active and standby states are repeated, the OP potential changes to a potential different from H and L depending on the repetition cycle. I will go there. In order to avoid this, as shown in Figure 4, φ 4 is applied only when the potential of OP is completely O L or O H.
Alternatively, this can be done by turning φ 3 ON and turning both Q 4 and Q 3 OFF when the OP potential changes.

第5図は本発明の他の実施例を示す。R5〜R7
は3個の高抵抗で、電源Vcc、Vss間に直列に接
続される。対向電極OPはスイツチングトランジ
スタQ3,Q4を介してノードN5,N6即ち抵抗R5
R6の直列接続点、抵抗R6とR7の直列接続点へ接
続される。トランジスタQ3,Q4のゲートへはク
ロツクA,φAが加えられ、ノードN5,N6はH,
Lレベル出力OH,OLを生じるから(R5〜R7の抵
抗値をそのように選ぶ)、第3図と同様な動作が
行なわれる。消費電力の点では第5図の方が第3
図より有利である。なお抵抗R1〜R7は拡散抵抗
などの他にトランジスタなどで構成してもよいこ
とは言う迄もない。
FIG. 5 shows another embodiment of the invention. R5R7
are three high resistances connected in series between the power supplies Vcc and Vss. The counter electrode OP connects to nodes N 5 and N 6 , that is, resistor R 5 via switching transistors Q 3 and Q 4 .
Connected to the series connection point of R 6 and the series connection point of resistors R 6 and R 7 . Clock A and φ A are applied to the gates of transistors Q 3 and Q 4 , and nodes N 5 and N 6 are at H,
Since the L level outputs O H and O L are generated (the resistance values of R 5 to R 7 are selected accordingly), the same operation as in FIG. 3 is performed. In terms of power consumption, Figure 5 ranks third.
This is more advantageous than the figure. It goes without saying that the resistors R 1 to R 7 may be composed of transistors or the like in addition to diffused resistors.

発明の効果 以上説明したように本発明では、高抵抗分圧回
路によりセルキヤパシタ対向電極に与える中間電
位を、メモリがアクテイブ、スタンバイを繰り返
し、この結果該対向電極がその寄生容量により与
えられるH,L電位に等しい2種の電位とし、該
分圧回路は該2種の電位を常時、同時に出力して
おり、その一方を選択して対向電極に印加するよ
うにしたので、選択と同時に当該電圧を対向電極
に加えることができ、高抵抗回路に不随する時定
数により該電圧印加が遅れるようなことがない。
Effects of the Invention As explained above, in the present invention, the memory repeatedly activates and standsby the intermediate potential applied to the cell capacitor counter electrode by the high resistance voltage divider circuit, and as a result, the counter electrode becomes The voltage dividing circuit always outputs the two potentials at the same time, and one of them is selected and applied to the opposite electrode, so that the voltage is applied at the same time as the selection. The voltage application can be applied to the counter electrode without delaying the voltage application due to time constants associated with high resistance circuits.

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

第1図は既提案方式を説明する回路図、第2図
はその動作説明用波形図、第3図は本発明の実施
例を示す回路図、第4図はその動作説明図、第5
図は他の実施例を示す回路である。 図面で、MCはメモリセル、Q1はそのトランジ
スタ、C1はキヤパシタ、OPは対向電極、Cp1
Cp2は寄生容量、VDは分圧回路、N3,M4はその
出力端、Vccは電源電圧、Vssは接地電位、であ
る。
FIG. 1 is a circuit diagram explaining the proposed method, FIG. 2 is a waveform diagram explaining its operation, FIG. 3 is a circuit diagram showing an embodiment of the present invention, FIG. 4 is a diagram explaining its operation, and FIG.
The figure shows a circuit showing another embodiment. In the drawing, MC is the memory cell, Q 1 is its transistor, C 1 is the capacitor, OP is the counter electrode, C p1 ,
C p2 is a parasitic capacitance, VD is a voltage dividing circuit, N 3 and M 4 are its output terminals, Vcc is a power supply voltage, and Vss is a ground potential.

Claims (1)

【特許請求の範囲】 1 トランジスタと、該トランジスタに一方の電
極が接続されたキヤパシタよりなる1トランジス
タ1キヤパシタ型ダイナミツク・メモリセルを備
え、前記キヤパシタの他方の電極には電源電圧よ
りも低い電圧が与えられる半導体記憶装置に於い
て、 前記電源電圧の略中間電圧よりも所定値だけ高
い第1電圧と、前記略中間電圧よりも所定値だけ
低い第2電圧を同時に出力可能な電圧発生回路
と、 スタンバイ時には前記第1電圧を、アクテイブ
時には前記第2電圧を、選択的に切り換えて前記
キヤパシタの他方の電極へ供給するスイツチング
素子と を具備することを特徴とする半導体記憶装置。
[Claims] A one-transistor, one-capacitor type dynamic memory cell consisting of a transistor and a capacitor having one electrode connected to the transistor, and the other electrode of the capacitor is connected to a voltage lower than the power supply voltage. In the provided semiconductor memory device, a voltage generating circuit capable of simultaneously outputting a first voltage higher by a predetermined value than a substantially intermediate voltage of the power supply voltage and a second voltage lower by a predetermined value than the substantially intermediate voltage; A semiconductor memory device comprising a switching element that selectively switches and supplies the first voltage to the other electrode of the capacitor during standby and the second voltage during active.
JP59067221A 1984-04-04 1984-04-04 Semiconductor memory device Granted JPS60211689A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59067221A JPS60211689A (en) 1984-04-04 1984-04-04 Semiconductor memory device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59067221A JPS60211689A (en) 1984-04-04 1984-04-04 Semiconductor memory device

Publications (2)

Publication Number Publication Date
JPS60211689A JPS60211689A (en) 1985-10-24
JPH0585990B2 true JPH0585990B2 (en) 1993-12-09

Family

ID=13338632

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59067221A Granted JPS60211689A (en) 1984-04-04 1984-04-04 Semiconductor memory device

Country Status (1)

Country Link
JP (1) JPS60211689A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2504140B2 (en) * 1988-10-14 1996-06-05 日本電気株式会社 MOS type dynamic semiconductor memory device

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6032981B2 (en) * 1977-04-04 1985-07-31 日本電気株式会社 binary storage device
JPH0219558A (en) * 1988-07-07 1990-01-23 Tokyo Kihan:Kk Impregnating device

Also Published As

Publication number Publication date
JPS60211689A (en) 1985-10-24

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