JPH1054865A - Specifying method for electrostatically broken down place in fet integrated circuit - Google Patents

Specifying method for electrostatically broken down place in fet integrated circuit

Info

Publication number
JPH1054865A
JPH1054865A JP8211686A JP21168696A JPH1054865A JP H1054865 A JPH1054865 A JP H1054865A JP 8211686 A JP8211686 A JP 8211686A JP 21168696 A JP21168696 A JP 21168696A JP H1054865 A JPH1054865 A JP H1054865A
Authority
JP
Japan
Prior art keywords
integrated circuit
fet
circuit
mos
static electricity
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.)
Pending
Application number
JP8211686A
Other languages
Japanese (ja)
Inventor
Masao Hoshino
雅夫 星野
Akio Iwabuchi
昭夫 岩渕
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.)
Sanken Electric Co Ltd
Original Assignee
Sanken Electric Co 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 Sanken Electric Co Ltd filed Critical Sanken Electric Co Ltd
Priority to JP8211686A priority Critical patent/JPH1054865A/en
Publication of JPH1054865A publication Critical patent/JPH1054865A/en
Pending legal-status Critical Current

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  • Testing Of Individual Semiconductor Devices (AREA)
  • Tests Of Electronic Circuits (AREA)
  • Metal-Oxide And Bipolar Metal-Oxide Semiconductor Integrated Circuits (AREA)

Abstract

PROBLEM TO BE SOLVED: To provide a specifying method in which a broken down place in an FET integrated circuit due to static electricity is specified easily. SOLUTION: A C-MOS inverter circuit 10 is replaced by a simple equivalent circuit 20 which contains capacitors 21 to 32 and a resistance 18, potential distributions in respective parts of the capacitors 21 to 32 are simulated and computed when a power-supply voltage is applied to the equivalent circuit 20, and potential distributions of respective MOS-FET's 11 to 16 inside the C-MOS inverter circuit 10 are given immediately before static electricity is applied. A place in which an overvoltage is applied is specified by the potential distributions, and the MOS-FET's 11 to 16 in which there is a possibility of being broken down electrostatically can be specified. Consequently, it is possible to easily specify a place which is broken down by static electricity in the C-MOS inverter circuit 10.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、FET(電界効果
トランジスタ)集積回路の静電気による破壊箇所を特定
する方法に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for specifying a broken portion of a FET (field effect transistor) integrated circuit due to static electricity.

【0002】[0002]

【従来の技術】最近、アッセンブリ(組立)工程等で発
生する摩擦などで静電気が発生して集積回路(IC)の
パッケ−ジ(外囲器)が帯電され、その帯電されたパッ
ケ−ジが何らかの原因で放電して集積回路内の各素子を
破損する所謂静電気破壊が集積回路の大規模化及び高密
度化に伴い多く発生している。この静電気破壊は、高速
でかつ高圧のインパルス電圧がパッケージから外部リー
ド端子を介して内部の集積回路に印加され、集積回路内
の各素子を構成するPN接合や酸化膜或いは各素子間の
配線膜等に大電流が流れて過大に発熱し、溶解して破壊
に至る場合が多い。このような静電気破壊(ESD)を
評価する方法としてパッケージ帯電法が従来から知られ
ており、また近年では静電気による集積回路の破壊箇所
等が等価回路のシミュレーション計算によりある程度推
測できるようになった。図3はパッケージ帯電法の試験
回路を示し、図3において、1は集積回路、1aはパッ
ケージ、2は外部リード端子、3は金属板、4は静電気
発生源としての印加電圧源、5はスイッチ、6は放電経
路上の物体の等価インピーダンスを示す。
2. Description of the Related Art Recently, static electricity is generated due to friction generated in an assembly process and the like, and a package (envelope) of an integrated circuit (IC) is charged, and the charged package is discharged. The so-called electrostatic destruction, in which each element in an integrated circuit is damaged by discharging for some reason, has occurred frequently as the scale and density of integrated circuits have increased. This electrostatic destruction occurs when a high-speed and high-voltage impulse voltage is applied from a package to an internal integrated circuit via an external lead terminal, and a PN junction or an oxide film constituting each element in the integrated circuit or a wiring film between the elements is formed. In many cases, a large current flows to generate excessive heat, melt and break down. As a method for evaluating such electrostatic discharge (ESD), a package charging method has been conventionally known. In recent years, a broken portion of an integrated circuit due to static electricity can be estimated to some extent by simulation calculation of an equivalent circuit. FIG. 3 shows a test circuit of the package charging method. In FIG. 3, 1 is an integrated circuit, 1a is a package, 2 is an external lead terminal, 3 is a metal plate, 4 is an applied voltage source as an electrostatic source, and 5 is a switch. , 6 indicate the equivalent impedance of the object on the discharge path.

【0003】[0003]

【発明が解決しようとする課題】しかしながら、集積回
路を構成する各素子がFET等の複雑な構造を有する素
子である場合、その等価回路が電流源や多数の容量性素
子及び抵抗素子等から構成されるため、集積回路全体と
しての等価回路が複雑となる。そのため、FET集積回
路に静電気が印加された場合におけるFET集積回路の
等価回路の各部の電位分布をシミュレーション計算によ
り求めることは極めて煩雑である。したがって、従来の
方法では静電気によるFET集積回路の破壊箇所を特定
することが極めて困難であった。
However, when each element constituting the integrated circuit is an element having a complicated structure such as an FET, its equivalent circuit is composed of a current source, a large number of capacitive elements, resistance elements, and the like. Therefore, the equivalent circuit of the entire integrated circuit becomes complicated. Therefore, when static electricity is applied to the FET integrated circuit, it is extremely complicated to obtain the potential distribution of each part of the equivalent circuit of the FET integrated circuit by simulation calculation. Therefore, it has been extremely difficult to specify a broken portion of the FET integrated circuit due to static electricity by the conventional method.

【0004】そこで、本発明はFET集積回路をコンデ
ンサを含む簡素な等価回路に置換することにより、FE
T集積回路の静電気による破壊箇所を容易に特定できる
方法を提供することを目的とする。
Therefore, the present invention replaces the FET integrated circuit with a simple equivalent circuit including a capacitor, thereby achieving FE
It is an object of the present invention to provide a method capable of easily specifying a broken portion of a T integrated circuit due to static electricity.

【0005】[0005]

【課題を解決するための手段】本発明によるFET集積
回路の静電気破壊箇所特定方法は、複数の端子を有する
FET集積回路の前記各端子間の静電容量を測定する過
程と、前記静電容量より前記FET集積回路をコンデン
サを含む等価回路に置換する過程と、前記等価回路に電
源電圧を印加した場合における前記等価回路の各部の電
位分布をシミュレーション計算により算出する過程と、
前記各部の電位分布より過大な電位の箇所を特定する過
程とを含む。
SUMMARY OF THE INVENTION According to the present invention, there is provided a method for identifying an electrostatic breakdown point of an FET integrated circuit, comprising the steps of: measuring a capacitance between the respective terminals of the FET integrated circuit having a plurality of terminals; Replacing the FET integrated circuit with an equivalent circuit including a capacitor, and calculating a potential distribution of each part of the equivalent circuit by a simulation calculation when a power supply voltage is applied to the equivalent circuit;
A step of specifying a location having an excessive potential from the potential distribution of each of the parts.

【0006】FET集積回路をコンデンサを含む簡素な
等価回路に置換し、等価回路に電源電圧を印加したとき
の等価回路の各部の電位分布をシミュレーション計算す
ることにより、静電気が印加される直前のFET集積回
路内の各素子の電位分布が与えられる。これらの電位分
布から過大電圧のかかる箇所を特定することにより、静
電気破壊される可能性がある素子を特定できる。したが
って、FET集積回路の静電気による破壊箇所を容易に
特定することができる。
[0006] The FET integrated circuit is replaced with a simple equivalent circuit including a capacitor, and the potential distribution of each part of the equivalent circuit when a power supply voltage is applied to the equivalent circuit is calculated by simulation. The potential distribution of each element in the integrated circuit is given. By specifying a location to which an excessive voltage is applied from these potential distributions, an element that may be damaged by static electricity can be specified. Therefore, it is possible to easily specify a broken portion of the FET integrated circuit due to static electricity.

【0007】[0007]

【発明の実施の形態】以下、本発明によるFET集積回
路の静電気破壊箇所特定方法の一実施形態を図1及び図
2に基づいて説明する。本実施形態で使用するFET集
積回路としてのC-MOS(相補形MOS)インバータ
回路10を図1に示す。図1のC-MOSインバータ回
路10では、PチャネルMOS-FET11〜13及び
NチャネルMOS-FET14〜16がそれぞれ一対に
接続されて3段のC-MOSインバータが形成されてい
る。図1において、17は浮遊容量、18は抵抗を示
し、電源電圧VDD及びVSSは通常はそれぞれ+5V及び
接地電位(0V)に固定されている。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of a method for specifying a portion where an electrostatic discharge is destroyed in an FET integrated circuit according to the present invention will be described below with reference to FIGS. FIG. 1 shows a C-MOS (complementary MOS) inverter circuit 10 as an FET integrated circuit used in the present embodiment. In the C-MOS inverter circuit 10 of FIG. 1, P-channel MOS-FETs 11 to 13 and N-channel MOS-FETs 14 to 16 are respectively connected in a pair to form a three-stage C-MOS inverter. In FIG. 1, reference numeral 17 denotes a stray capacitance, reference numeral 18 denotes a resistor, and power supply voltages V DD and V SS are normally fixed at +5 V and ground potential (0 V), respectively.

【0008】次に、図1に示すC-MOSインバータ回
路10の静電気破壊箇所の特定方法について説明する。
まず、C-MOSインバータ回路10におけるPチャネ
ルMOS-FET11〜13及びNチャネルMOS-FE
T14〜16のゲート−ソース端子間及びゲート−ドレ
イン端子間の静電容量をそれぞれ静電容量計等で測定す
る。続いて、PチャネルMOS-FET11〜13及び
NチャネルMOS-FET14〜16のゲート−ソース
端子間及びゲート−ドレイン端子間のそれぞれの静電容
量の測定値に基づいて図1に示すC-MOSインバータ
回路10のPチャネルMOS-FET11〜13及びN
チャネルMOS-FET14〜16及び抵抗18を図2
に示すようにコンデンサ21〜32及び抵抗18から成
る等価回路20に置き換える。その後、SPICE等の
回路シミュレーション用プログラムを内蔵した計算機
(回路シミュレータ)を使用して等価回路20に一定の
電源電圧VDD=+5V及びVSS=0Vを印加した場合の
等価回路20の各点(図2のA点〜D点等)の電位をシ
ミュレーション計算により算出する。このとき、例えば
各コンデンサ25〜32の静電容量がC-MOSインバ
ータ回路10の浮遊容量17より極めて小さいならば、
浮遊容量17のインピーダンスが極めて小さいことを意
味するから、C点の電位は限りなくVSS=0Vに近づ
く。したがって、この場合はコンデンサ29の両端の電
圧が略5Vとなるから、PチャネルMOS-FET13
のゲート−ソース端子間に極めて過大な電圧がかかるこ
とがわかる。よって、静電気破壊を受ける可能性が最も
高い素子はPチャネルMOS-FET13と特定でき
る。なお、本発明者は本実施形態で特定したC-MOS
インバータ回路10の破壊箇所と図3に示すパッケージ
帯電法により本実施形態と同様の条件下でC-MOSイ
ンバータ回路10に静電気を印加したときの実際の破壊
箇所が一致することを実験で確認した。
Next, a description will be given of a method of specifying a portion where static electricity is destroyed in the C-MOS inverter circuit 10 shown in FIG.
First, the P-channel MOS-FETs 11 to 13 and the N-channel MOS-FE in the C-MOS inverter circuit 10
The capacitance between the gate and the source terminal and between the gate and the drain terminal of T14 to T16 are measured with a capacitance meter or the like. Subsequently, based on the measured values of the capacitance between the gate and the source terminal and between the gate and the drain terminal of the P-channel MOS-FETs 11 to 13 and the N-channel MOS-FETs 14 to 16, the C-MOS inverter shown in FIG. P-channel MOS-FETs 11 to 13 and N of circuit 10
The channel MOS-FETs 14 to 16 and the resistor 18 are shown in FIG.
Is replaced by an equivalent circuit 20 including capacitors 21 to 32 and a resistor 18 as shown in FIG. After that, when a constant power supply voltage V DD = + 5 V and V SS = 0 V are applied to the equivalent circuit 20 using a computer (circuit simulator) incorporating a circuit simulation program such as SPICE, each point of the equivalent circuit 20 ( The potential at points A to D in FIG. 2) is calculated by simulation calculation. At this time, for example, if the capacitance of each of the capacitors 25 to 32 is extremely smaller than the stray capacitance 17 of the C-MOS inverter circuit 10,
Since the impedance of the stray capacitance 17 is extremely small, the potential at the point C approaches V SS = 0 V without limit. Therefore, in this case, the voltage across the capacitor 29 becomes approximately 5 V, so that the P-channel MOS-FET 13
It can be seen that an extremely large voltage is applied between the gate and source terminals of FIG. Therefore, the element most likely to be damaged by static electricity can be specified as the P-channel MOS-FET 13. Note that the present inventor has identified the C-MOS specified in the present embodiment.
It was confirmed by experiments that the destruction point of the inverter circuit 10 and the actual destruction point when static electricity was applied to the C-MOS inverter circuit 10 under the same conditions as in the present embodiment by the package charging method shown in FIG. .

【0009】本実施形態では、C-MOSインバータ回
路10をコンデンサ21〜32及び抵抗18から成る簡
素な等価回路20に置換し、等価回路20に電源電圧V
DD、VSSを印加した場合におけるコンデンサ21〜32
の電位分布をシミュレーション計算することにより、静
電気が印加される直前のC-MOSインバータ回路10
内の各MOS-FET11〜16の電位分布が与えられ
る。これらの電位分布から過大電圧のかかる箇所を特定
することにより、静電気破壊される可能性が最も高いM
OS-FETを特定できる。したがって、C-MOSイン
バータ回路10の静電気による破壊箇所を容易に特定す
ることができ、また、これによって静電気破壊を受け易
い箇所における素子の対策変更を回路設計の段階にて行
うことが可能となる。
In this embodiment, the C-MOS inverter circuit 10 is replaced with a simple equivalent circuit 20 composed of capacitors 21 to 32 and a resistor 18, and the equivalent circuit 20 has a power supply voltage V
DD, the capacitor in the case of applying the V SS 21~32
Of the C-MOS inverter circuit 10 immediately before the static electricity is applied by calculating the potential distribution of the
Of the respective MOS-FETs 11 to 16 are given. By specifying a location where an excessive voltage is applied from these potential distributions, M
OS-FET can be specified. Therefore, the location where the C-MOS inverter circuit 10 is destroyed by the static electricity can be easily specified, and the countermeasure change of the element in the location susceptible to the electrostatic breakdown can be made at the circuit design stage. .

【0010】本発明の実施態様は上記の実施形態に限定
されず、種々の変更が可能である。例えば、上記の実施
形態ではFET集積回路としてC-MOSインバータ回
路を使用した場合を示したが、C-MOSインバータ回
路に限らず、AND(論理積)ゲート、OR(論理和)
ゲート等の他のMOS-FET集積回路或いはMOS-F
ET以外の他の絶縁ゲート形FETの集積回路にも適用
が可能である。また、上記の実施形態ではFET集積回
路がMOS-FET及び抵抗で構成された場合を示した
が、抵抗が無い場合でもよく、更にMOS-FET以外
の絶縁ゲート形FET又はコンデンサ、コイル等の受動
素子を含んでもよい。
[0010] Embodiments of the present invention are not limited to the above embodiments, and various modifications are possible. For example, in the above-described embodiment, the case where the C-MOS inverter circuit is used as the FET integrated circuit has been described. However, the present invention is not limited to the C-MOS inverter circuit.
Other MOS-FET integrated circuits such as gates or MOS-F
The present invention can be applied to an insulated gate FET integrated circuit other than ET. In the above embodiment, the case where the FET integrated circuit is constituted by the MOS-FET and the resistor is shown. However, the case where there is no resistor may be employed. Elements may be included.

【0011】[0011]

【発明の効果】本発明によれば、コンデンサを含む簡素
な等価回路のシミュレーション計算によりFET集積回
路の静電気による破壊箇所を容易に特定することができ
るので、FET集積回路の仕様が決定した時点で静電気
破壊を受け易い箇所を予め特定し、その箇所について対
策変更を行うことにより、アッセンブリ工程におけるF
ET集積回路の静電気破壊を未然に防止することが可能
となる。特に、LSI(大規模集積回路)等の多素子で
かつ高密度の集積回路において本発明の効果が顕著であ
る。
According to the present invention, it is possible to easily specify a portion of a FET integrated circuit that is destroyed by static electricity by a simulation calculation of a simple equivalent circuit including a capacitor. By identifying in advance the locations that are susceptible to electrostatic damage and changing the countermeasures for those locations, the F in the assembly process can be reduced.
This makes it possible to prevent electrostatic breakdown of the ET integrated circuit. In particular, the effects of the present invention are remarkable in a multi-element and high-density integrated circuit such as an LSI (large-scale integrated circuit).

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

【図1】 本発明の一実施形態で使用するC-MOSイ
ンバータ回路を示す電気回路図
FIG. 1 is an electric circuit diagram showing a C-MOS inverter circuit used in an embodiment of the present invention.

【図2】 図1に示すC-MOSインバータ回路のコン
デンサ等価回路を示す電気回路図
FIG. 2 is an electric circuit diagram showing a capacitor equivalent circuit of the C-MOS inverter circuit shown in FIG.

【図3】 パッケージ帯電法の概略を示す試験回路図FIG. 3 is a test circuit diagram schematically showing a package charging method.

【符号の説明】[Explanation of symbols]

1...集積回路、1a...パッケージ、2...外
部リード端子、3...金属板、4...印加電圧源、
5...スイッチ、6...等価インピーダンス、1
0...C-MOSインバータ回路(FET集積回
路)、11〜13...PチャネルMOS-FET、1
4〜16...NチャネルMOS-FET、17...
浮遊容量、18...抵抗、20...等価回路、21
〜32...コンデンサ
1. . . Integrated circuit, 1a. . . Package 2. . . 2. external lead terminals; . . 3. metal plate; . . Applied voltage source,
5. . . Switch, 6. . . Equivalent impedance, 1
0. . . C-MOS inverter circuit (FET integrated circuit), 11-13. . . P-channel MOS-FET, 1
4-16. . . N-channel MOS-FET, 17. . .
Stray capacitance, 18. . . Resistance, 20. . . Equivalent circuit, 21
~ 32. . . Capacitor

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 複数の端子を有するFET集積回路の前
記各端子間の静電容量を測定する過程と、 前記静電容量より前記FET集積回路をコンデンサを含
む等価回路に置換する過程と、 前記等価回路に電源電圧を印加した場合における前記等
価回路の各部の電位分布をシミュレーション計算により
算出する過程と、 前記各部の電位分布より過大な電位の箇所を特定する過
程と、を含むことを特徴とするFET集積回路の静電気
破壊箇所特定方法。
A step of measuring a capacitance between the respective terminals of the FET integrated circuit having a plurality of terminals; a step of replacing the FET integrated circuit with an equivalent circuit including a capacitor from the capacitance; A step of calculating a potential distribution of each part of the equivalent circuit when a power supply voltage is applied to the equivalent circuit by a simulation calculation; anda step of specifying a location of a potential which is excessive than the potential distribution of each part. Method for specifying the location of an electrostatic breakdown in a FET integrated circuit.
JP8211686A 1996-08-09 1996-08-09 Specifying method for electrostatically broken down place in fet integrated circuit Pending JPH1054865A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8211686A JPH1054865A (en) 1996-08-09 1996-08-09 Specifying method for electrostatically broken down place in fet integrated circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8211686A JPH1054865A (en) 1996-08-09 1996-08-09 Specifying method for electrostatically broken down place in fet integrated circuit

Publications (1)

Publication Number Publication Date
JPH1054865A true JPH1054865A (en) 1998-02-24

Family

ID=16609913

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8211686A Pending JPH1054865A (en) 1996-08-09 1996-08-09 Specifying method for electrostatically broken down place in fet integrated circuit

Country Status (1)

Country Link
JP (1) JPH1054865A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007073838A (en) * 2005-09-08 2007-03-22 Matsushita Electric Ind Co Ltd Electrostatic noise tolerance analysis method for semiconductor integrated circuit device and design optimization method for semiconductor integrated circuit device using the same

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007073838A (en) * 2005-09-08 2007-03-22 Matsushita Electric Ind Co Ltd Electrostatic noise tolerance analysis method for semiconductor integrated circuit device and design optimization method for semiconductor integrated circuit device using the same

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