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JPH0140504B2 - - Google Patents
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JPH0140504B2 - - Google Patents

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Publication number
JPH0140504B2
JPH0140504B2 JP56102565A JP10256581A JPH0140504B2 JP H0140504 B2 JPH0140504 B2 JP H0140504B2 JP 56102565 A JP56102565 A JP 56102565A JP 10256581 A JP10256581 A JP 10256581A JP H0140504 B2 JPH0140504 B2 JP H0140504B2
Authority
JP
Japan
Prior art keywords
region
type
well
conductivity type
charge
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
Application number
JP56102565A
Other languages
Japanese (ja)
Other versions
JPS584967A (en
Inventor
Nobuo Sasaki
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 JP56102565A priority Critical patent/JPS584967A/en
Publication of JPS584967A publication Critical patent/JPS584967A/en
Publication of JPH0140504B2 publication Critical patent/JPH0140504B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10BELECTRONIC MEMORY DEVICES
    • H10B12/00Dynamic random access memory [DRAM] devices

Landscapes

  • Semiconductor Memories (AREA)

Description

【発明の詳細な説明】 本発明は、チヤージ・ポンプ作用で電荷の蓄積
を行ない、それに依るトランジスタの閾値電圧変
化を情報の“1”或いは“0”に対応させる形式
の半導体記憶装置の改良に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement in a semiconductor memory device in which charges are accumulated by a charge pump action, and the resulting change in threshold voltage of a transistor corresponds to information "1" or "0". .

本発明者は、さきに、チヤージ・ポンピング・
メモリと称し、第1図に見られるような半導体記
憶装置を提供した。
The present inventor has previously discovered that charge pumping
A semiconductor storage device called a memory as shown in FIG. 1 was provided.

図に於いて、1はサフアイアなどの単結晶絶縁
基板、2は良好なエピタキシヤル成長を行なう為
のバツフア層的作用をするn+型シリコン半導体
層、3はp型シリコン半導体層、4は二酸化シリ
コン絶縁分離層、5はゲート絶縁膜、6はn+
多結晶シリコン・ゲート電極、7及び8はp+
遮蔽領域、9はn+型ソース領域、10はn+型ド
レイン領域をそれぞれ示す。
In the figure, 1 is a single-crystal insulating substrate such as sapphire, 2 is an n + type silicon semiconductor layer that acts as a buffer layer for good epitaxial growth, 3 is a p-type silicon semiconductor layer, and 4 is carbon dioxide. A silicon insulation separation layer, 5 a gate insulating film, 6 an n + type polycrystalline silicon gate electrode, 7 and 8 a p + type shielding region, 9 an n + type source region, and 10 an n + type drain region, respectively. show.

この装置では、ソース領域9及びドレイン領域
10間に電圧を印加しておき、ゲート電極6にも
電圧を印加するとチヤネルが形成され電流が流れ
る。そして、ゲート電極6の電位を急激に零にす
ると、電子がp型シリコン半導体層3に注入され
そこに負の電荷が蓄積される。これに依り、ソー
ス領域9からドレイン領域10に至る電流パスに
於ける閾値電圧は変化する。そこで、この閾値電
圧の変化をセンスしてやれば情報の書き込みの有
無を読み出すことができる。
In this device, a voltage is applied between the source region 9 and the drain region 10, and when a voltage is also applied to the gate electrode 6, a channel is formed and a current flows. Then, when the potential of the gate electrode 6 is suddenly reduced to zero, electrons are injected into the p-type silicon semiconductor layer 3 and negative charges are accumulated therein. As a result, the threshold voltage in the current path from source region 9 to drain region 10 changes. Therefore, by sensing the change in this threshold voltage, it is possible to read whether information has been written.

ところで、前記装置は、基板1がサフアイアで
ある為、シリコンの基板に比較すると甚だ高価で
あり、また、その上にエピタキシヤル成長させた
シリコン半導体層も充分に良質とは云い難い。
By the way, since the substrate 1 of the device is made of sapphire, it is extremely expensive compared to a silicon substrate, and the silicon semiconductor layer epitaxially grown thereon is also of insufficient quality.

そこで、第2図に見られる改良装置を提供し
た。
Therefore, an improved device as shown in FIG. 2 was provided.

図に於いて、11はn型シリコン半導体基板、
12はフイールド用二酸化シリコン絶縁膜、13
はp型ウエル、14は再結合中心領域、15はゲ
ート絶縁膜、16はn+型多結晶シリコン・ゲー
ト電極、17はn+型ソース領域、18はn+型ド
レイン領域をそれぞれ示す。
In the figure, 11 is an n-type silicon semiconductor substrate;
12 is a silicon dioxide insulating film for the field, 13
14 is a p-type well, 14 is a recombination center region, 15 is a gate insulating film, 16 is an n + type polycrystalline silicon gate electrode, 17 is an n + type source region, and 18 is an n + type drain region.

この装置が第1図装置と相違する点は、基板1
1がシリコン半導体であること、基板11内にp
型ウエル13を形成し、そこに電荷を蓄積するよ
うにしたこと、この電荷の蓄積は、チヤージ・ポ
ンピング効果でp型ウエル13内に注入された電
子が再結合中心領域14に於いて正孔と結合する
のでp型ウエル13内の正孔が減少し、結果的に
電荷の蓄積が行なわれる。ところが、このように
再結合中心領域14を形成するとp型ウエル13
内に蓄積された電荷が漏洩し易くなることにも結
び付くので長時間の電荷の蓄積を行なうことがで
きない。
The difference between this device and the device shown in FIG. 1 is that the substrate 1
1 is a silicon semiconductor, and p is in the substrate 11.
The type well 13 is formed and charge is accumulated therein. This charge accumulation is caused by the charge pumping effect when electrons injected into the p-type well 13 become holes in the recombination center region 14. As a result, the number of holes in the p-type well 13 decreases, and as a result, charges are accumulated. However, when the recombination center region 14 is formed in this way, the p-type well 13
This also leads to the possibility that the charges accumulated within the capacitor tend to leak, making it impossible to accumulate charges for a long period of time.

本発明は、サフアイアなどの単結晶絶縁基板に
比較して安価なシリコン半導体基板を用い、しか
も、電荷の蓄積性を良好にするものであり、以下
これを詳細に説明する。
The present invention uses a silicon semiconductor substrate, which is cheaper than a single crystal insulating substrate such as sapphire, and has good charge storage properties, and will be described in detail below.

第3図は本発明一実施例の要部断面説面図であ
る。
FIG. 3 is an explanatory sectional view of a main part of an embodiment of the present invention.

図に於いて、21はn型シリコン半導体基板、
22はフイールド用二酸化シリコン絶縁膜、23
はp+型遮蔽領域、24はn型電荷捕捉領域、2
5はp型ウエル、26はゲート絶縁膜、27は
n+型多結晶シリコン・ゲート電極、28,29
はp+型遮蔽領域、30はn+型ソース領域、31
はn+型ドレイン領域、32は燐硅酸ガラス絶縁
膜、33はソース電極、34はドレイン電極をそ
れぞれ示す。
In the figure, 21 is an n-type silicon semiconductor substrate;
22 is a silicon dioxide insulating film for the field, 23
is a p + type shielding region, 24 is an n-type charge trapping region, 2
5 is a p-type well, 26 is a gate insulating film, and 27 is a p-type well.
n + type polycrystalline silicon gate electrode, 28, 29
is a p + type shielding region, 30 is an n + type source region, 31
3 is an n + type drain region, 32 is a phosphosilicate glass insulating film, 33 is a source electrode, and 34 is a drain electrode.

この実施例では、第2図に見られるような再結
合中心領域はなく、その代り、p型ウエル25の
底面を覆うn型電荷捕捉領域24が形成されてい
る。従つて、チヤージ・ポンピング効果でp型ウ
エル25内に注入された電子はn型電荷捕捉領域
24にトラツプされ、漏洩は極めて少なくなる。
即ち、ゲート電極27に電圧を印加することに依
つてソース領域30及びドレイン領域31間に生
成された反転層よりp型ウエル25内にチヤー
ジ・ポンプされた電子はポテンシヤルの低いn型
電荷捕捉領域24にトラツプされ、これに依り、
n型電荷捕捉領域24とp型ウエル25とは順方
向にバイアスされるので、p・n接合ダイオード
の立ち上り分を無視すれば、両者は等電位とな
る。これはn型電荷捕捉領域24だけでなくp型
ウエル25も負にバイアスされることであり、従
つて、ソース領域30及びドレイン領域31間の
電流通路に於ける閾値電圧は変化することにな
る。そこで、この変化を従来装置と同様に情報の
“1”、“0”に対応させれば良い。
In this embodiment, there is no recombination center region as seen in FIG. 2, but instead an n-type charge trapping region 24 is formed that covers the bottom surface of the p-type well 25. Therefore, electrons injected into the p-type well 25 due to the charge pumping effect are trapped in the n-type charge trapping region 24, and leakage is extremely reduced.
That is, by applying a voltage to the gate electrode 27, electrons charge-pumped into the p-type well 25 from the inversion layer generated between the source region 30 and the drain region 31 are transferred to a low-potential n-type charge trapping region. 24, and as a result,
Since the n-type charge trapping region 24 and the p-type well 25 are biased in the forward direction, they have the same potential if the rise of the p-n junction diode is ignored. This means that not only the n-type charge trapping region 24 but also the p-well 25 will be negatively biased, and therefore the threshold voltage in the current path between the source region 30 and the drain region 31 will change. . Therefore, this change should be made to correspond to the information "1" and "0" as in the conventional device.

前記実施例の製造は容易であり、例えばp+
遮蔽領域23、n型電荷捕捉領域24、p型ウエ
ル25はフイールド用二酸化シリコン絶縁膜22
をマスクにしてイオン注入及び拡散に依つて形成
でき、また、他の部分は通常のMIS電界効果トラ
ンジスタを形成する工程と殆んど変りない。次
に、本実施例の具体的数値例を挙げる。
The manufacturing of the above embodiment is easy; for example, the p + type shielding region 23, the n-type charge trapping region 24, and the p-type well 25 are formed by forming the silicon dioxide insulating film 22 for the field.
It can be formed by ion implantation and diffusion using a mask, and the other parts are almost the same as the process for forming a normal MIS field effect transistor. Next, specific numerical examples of this example will be given.

絶縁膜22の厚さ:6000〔Å〕 領域23の厚さ:3000〔Å〕 領域23の不純物濃度:2×1016〔cm-3〕 領域24の厚さ:3000〔Å〕 領域24の不純物濃度:4×1015〔cm-3〕 領域の深さ:1〔μm〕 領域25の不純物濃度:1×1016〔cm-3〕 絶縁膜26の厚さ:400〔Å〕 電極27の厚さ:4000〔Å〕 領域28,29の厚さ:3000〔Å〕 領域28,29の不純物濃度:2×1016〔cm-3〕 領域30,31の深さ:3000〔Å〕 領域30,31の不純物濃度:1×1020〜21〔cm-3〕 以上の説明で判るように、本発明に依れば、ソ
ース領域とドレイン領域間に生成されるチヤネル
から電荷が注入されるウエルの下面をウエルと反
対導電型の電荷捕捉領域を形成するとともに更に
その下面をウエルと同導電型の遮蔽領域で覆つて
あるので、基板として安価な半導体を使用してい
るにも拘わらず、蓄積電荷の漏洩は極めて少なく
することができる。
Thickness of insulating film 22: 6000 [Å] Thickness of region 23: 3000 [Å] Impurity concentration of region 23: 2×10 16 [cm -3 ] Thickness of region 24: 3000 [Å] Impurity of region 24 Concentration: 4×10 15 [cm -3 ] Region depth: 1 [μm] Impurity concentration in region 25: 1×10 16 [cm -3 ] Thickness of insulating film 26: 400 [Å] Thickness of electrode 27 Thickness of regions 28 and 29: 3000 [Å] Impurity concentration of regions 28 and 29: 2×10 16 [cm -3 ] Depth of regions 30 and 31: 3000 [Å] Region 30, Impurity concentration of 31: 1×10 20 to 21 [cm -3 ] As can be seen from the above explanation, according to the present invention, the well where charges are injected from the channel generated between the source region and the drain region. A charge trapping region of the opposite conductivity type to that of the well is formed on the lower surface, and the lower surface is further covered with a shielding region of the same conductivity type as the well, so that even though an inexpensive semiconductor is used as the substrate, accumulated charges can be prevented. leakage can be extremely reduced.

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

第1図及び第2図は従来例の要部断面説明図、
第3図は本発明一実施例の要部断面説明図であ
る。 図において、21は基板、22は絶縁膜、23
は遮蔽領域、24は電荷捕捉領域、25はウエ
ル、26はゲート絶縁膜、27はゲート電極、2
8,29は遮蔽領域、30はソース領域、31は
ドレイン領域である。
Figures 1 and 2 are cross-sectional explanatory diagrams of main parts of the conventional example;
FIG. 3 is an explanatory sectional view of a main part of an embodiment of the present invention. In the figure, 21 is a substrate, 22 is an insulating film, and 23
24 is a shielding region, 24 is a charge trapping region, 25 is a well, 26 is a gate insulating film, 27 is a gate electrode, 2
8 and 29 are shield regions, 30 is a source region, and 31 is a drain region.

Claims (1)

【特許請求の範囲】[Claims] 1 一導電型の半導体基板に電気的にフロートし
ている反対導電型のウエルを形成し、そのウエル
内に相対向して形成された一導電型の領域間に生
成される反転層からチヤージ・ポンプ作用で電荷
をウエルに注入し、前記一導電型の領域間に反転
層を生成する為の閾値電圧を変化させる形式の半
導体記憶装置に於いて、前記ウエルの下面を覆う
一導電型電荷捕捉領域及びその電荷捕捉領域の下
面を覆う反対導電型遮蔽領域を備えてなることを
特徴とする半導体記憶装置。
1. An electrically floating well of an opposite conductivity type is formed in a semiconductor substrate of one conductivity type, and charge is generated from an inversion layer generated between regions of one conductivity type formed oppositely in the well. In a semiconductor memory device of the type in which charges are injected into a well by a pump action and a threshold voltage is varied to generate an inversion layer between the regions of one conductivity type, charge trapping of one conductivity type covers the bottom surface of the well. What is claimed is: 1. A semiconductor memory device comprising a region and a shielding region of an opposite conductivity type covering a lower surface of the charge trapping region.
JP56102565A 1981-06-30 1981-06-30 Semiconductor memory storage Granted JPS584967A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56102565A JPS584967A (en) 1981-06-30 1981-06-30 Semiconductor memory storage

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56102565A JPS584967A (en) 1981-06-30 1981-06-30 Semiconductor memory storage

Publications (2)

Publication Number Publication Date
JPS584967A JPS584967A (en) 1983-01-12
JPH0140504B2 true JPH0140504B2 (en) 1989-08-29

Family

ID=14330737

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56102565A Granted JPS584967A (en) 1981-06-30 1981-06-30 Semiconductor memory storage

Country Status (1)

Country Link
JP (1) JPS584967A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1988008617A1 (en) * 1987-04-20 1988-11-03 Research Corporation Technologies, Inc. Buried well dram
US5197336A (en) * 1990-01-29 1993-03-30 Fuji Electric Co., Ltd. Karman vortex flow meter

Also Published As

Publication number Publication date
JPS584967A (en) 1983-01-12

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