JPS5921169B2 - Failure analysis method for semiconductor devices - Google Patents
Failure analysis method for semiconductor devicesInfo
- Publication number
- JPS5921169B2 JPS5921169B2 JP713477A JP713477A JPS5921169B2 JP S5921169 B2 JPS5921169 B2 JP S5921169B2 JP 713477 A JP713477 A JP 713477A JP 713477 A JP713477 A JP 713477A JP S5921169 B2 JPS5921169 B2 JP S5921169B2
- Authority
- JP
- Japan
- Prior art keywords
- junction region
- junction
- liquid crystal
- field effect
- crystal film
- 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.)
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- Testing Or Measuring Of Semiconductors Or The Like (AREA)
Description
【発明の詳細な説明】
本発明は半導体素子の不良解析法に係り、とくにPN接
合領域の接合性の良否解析法に係る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a failure analysis method for semiconductor devices, and particularly to a method for analyzing the quality of bonding in a PN junction region.
半導体素子は周知の如く、半導体に導電型決定が異る少
なくとも2種の不純物を含有するPN接合領域が基本と
なつて構成されている。そしてこのPN接合領域に課せ
られた重要な電気的特性のひとつとして逆方向特性があ
る。これはPN接合に逆方向電圧を与えたときの逆方向
電圧と逆方向電流の関係であるが、逆方向電流が規定の
電流値を超過すると、PN接合リーク電流として半導体
素子が動作しない不良原因となる。半導体素子の不良原
因となるリーク電流にはPN接合リーク電流以外に、絶
縁膜のピンホールに起因するリーク電流などもある。し
たがつて半導体素子をブラックボックスとして調べた時
のリーク電流は、PN接合リーク電流によるのか、絶縁
膜のピンホールに起因するリーク電流などによるのか区
別しがたい。そこで最終的に絶縁膜等を除去して、PN
接合領域だけを解析する必要か生じる。この最終的にP
N接合領域だけを解析する方法として、従来、PN接合
領域に金属電極を形成せしめてこれと半導体基板との逆
方向特性を調べるとか、PN接合領域に電子ビームを照
射し、PN接合領域またはその近傍に形成せしめた金属
電極から電子ビーム誘起電流を取出して調べるなどの方
法がよく知られている。しかしこれら従来の解析方法に
はいずれも欠点がある。すなわちこれら従来の方法では
PN接合領域またはその近傍への金属電極を形成し、か
つそこへの探針接触を必要とすることである。半導体素
子とくに集積回路など高集積化高密度化された半導体素
子では、その半導体素子内には幾千幾万の微細なパター
ン寸法のPN接合領域が作り込まれている。このような
微細なパターン寸法、たとえば幾μm角のようなパター
ン領域のPN接合領域内に金属電極を形成することは、
半・ 導体素子製造プロセス上はともかく、不良解析対
象の試料にはパッケージ等が設けられているのが通常で
あつて公知の写真製版技術を適用できず極めて困難であ
る。また微小電極への電気接続を得るための探針接触は
、ウエハプローバでよく経験門 されているように難か
しい。また、従来、上記欠点を解消するようにした解析
法として、特開昭50−134379号公報に記載され
ているような方法があつた。As is well known, a semiconductor element basically consists of a PN junction region containing at least two types of impurities having different conductivity types in a semiconductor. One of the important electrical characteristics imposed on this PN junction region is reverse direction characteristics. This is the relationship between the reverse voltage and reverse current when a reverse voltage is applied to the PN junction, but if the reverse current exceeds the specified current value, it will become a PN junction leak current, which will cause the semiconductor device to malfunction. becomes. Leakage currents that cause defects in semiconductor devices include, in addition to PN junction leakage currents, leakage currents caused by pinholes in insulating films. Therefore, when examining a semiconductor element as a black box, it is difficult to distinguish whether the leakage current is due to a PN junction leakage current or a leakage current due to a pinhole in an insulating film. Therefore, the insulating film etc. are finally removed and the PN
It may become necessary to analyze only the joint area. In this final P
Conventionally, methods for analyzing only the N-junction region include forming a metal electrode in the PN-junction region and examining the reverse characteristics between this and the semiconductor substrate, or irradiating the PN-junction region with an electron beam to analyze the PN-junction region or its surroundings. A well-known method is to extract and examine the electron beam induced current from a metal electrode formed nearby. However, all of these conventional analysis methods have drawbacks. That is, these conventional methods require the formation of a metal electrode at or near the PN junction region and the need for probe contact thereto. BACKGROUND ART In semiconductor devices, especially highly integrated and highly dense semiconductor devices such as integrated circuits, tens of thousands of PN junction regions with fine pattern dimensions are built into the semiconductor device. Forming a metal electrode in the PN junction region of such a fine pattern area, for example, a pattern area several μm square, is
Regardless of the manufacturing process of semiconductor/conductor elements, the sample to be analyzed for failure usually has a package, etc., making it extremely difficult to apply known photolithography techniques. Furthermore, contacting the probe to obtain electrical connection to the microelectrode is difficult, as is often the case with wafer probers. Furthermore, conventionally, as an analysis method designed to eliminate the above-mentioned drawbacks, there has been a method described in Japanese Patent Application Laid-open No. 134379/1983.
これはPN接合領域上に液晶層及びガラス板を設け、こ
れらを通して偏光された光を連続的にPN接合領域上に
投射し、液晶層中の複屈折的変化を視覚的に観察するよ
うにしたものであつた。しかしなから上記従来方法では
、PN接合りーク電流が他の電気回路に悪影響を与え、
そのため正確な解析、検査かできない欠点があり、また
液晶の電界効果が弱まつて検査、解析か困難となる欠点
かあつた。In this method, a liquid crystal layer and a glass plate were provided on the PN junction area, and polarized light was continuously projected onto the PN junction area through these layers, allowing the birefringence changes in the liquid crystal layer to be visually observed. It was hot. However, in the above conventional method, the PN junction leakage current adversely affects other electric circuits,
Therefore, it had the disadvantage that accurate analysis and inspection could not be done, and the electric field effect of the liquid crystal weakened, making inspection and analysis difficult.
本発明は、上記従来方法の欠点を除去するためになされ
たもので、PN接合領域上に電界効果型液晶膜及びガラ
ス板を設け、これらを通して上記PN接合領域に偏光さ
れた光と偏光されていない光とを同時に重複して、かつ
断続的に投射することにより、他の電気回路への悪影響
がなく、かつ液晶膜の電界効果を弱めることのない半導
体素子の不良解析法を提供することを目的としている。The present invention was made in order to eliminate the drawbacks of the above-mentioned conventional method, and a field-effect liquid crystal film and a glass plate are provided on the PN junction region, and the polarized light and the polarized light are transmitted through these to the PN junction region. To provide a failure analysis method for semiconductor devices that does not have an adverse effect on other electric circuits and does not weaken the electric field effect of a liquid crystal film by simultaneously and overlappingly and intermittently projecting light that is The purpose is
以下、図面を参照しながら本発明による解析法について
述べる。第1図は本発明による解析法を説明するための
工程別断面図であつて、解析の対象とするPN接合領域
1のみの部分を取上げてあり、絶縁膜、メタライゼーシ
ヨン等は除去してある。The analysis method according to the present invention will be described below with reference to the drawings. FIG. 1 is a process-by-step cross-sectional view for explaining the analysis method according to the present invention, and shows only the PN junction region 1, which is the subject of analysis, and the insulating film, metallization, etc. are not removed. There is.
絶縁膜、メタラィゼーシヨン等の除去されたPN接合領
域1の解析によつて真にPN接合の欠陥にもとずくリー
ク電流かどうかの判定ができる。第1図aは半導体基板
2にPN接合領域1か露出している状態を示している。
本発明による解析法では、このPN接合領域1の露出し
た半導体基板2の半導体基板主面2aの上を電界効果型
結晶膜3で被覆し(第1図b)、つづいてガラス板4を
前記電界効果型液晶膜3の上に載置する。電界効果型液
晶膜3の被覆範囲およびガラス板4の形状大きさは、解
析の対象としているPN接合領域1を充分にカバーでき
る形状、大きさとする(第1図c)。つづいて第2図に
示すごとく、電界効果液晶膜3、ガラス板4の設けられ
た試料100を光学系200のもとに配置する。光学系
200は、光源5からの光を偏光子6で偏光した光7を
上記PN接合領域1に投射するためのものである。光源
5″からの偏光されない通常光7′もPN接合領域1に
投射するか、この通常光7″は、偏光された光7の光路
とは異なり、直接に試料100面へ斜めから入射してP
N接合領域1を照射し、試料100面で整反射されて射
出する。したがつて、通常光7″は接眼レンズ11を通
過しない。これに対し、偏光された光7は、プリズム8
、対物レンズ9、ガラス板4、電解効果型液晶膜3を通
過してPN接合領域1へ至り、そこで反射される。そし
て再び反射光は、電界効果型液晶膜3、ガラス板4、対
物レンズ9を通過しプリズム8に至る。プリズム8は半
透明鏡であり、反射後の偏光された光7は直進し、検光
子10、接眼レンズ11を通過して人間の眼またはテレ
ビカメラで観察される。対物レンズ9,接眼レンズ11
は微小な寸法のPN接合領域1を拡大して詳細観察でき
るようにするために設けられている。偏光子6と検光子
10の偏光面に関する相対関係が、反射後の偏光された
光7等を遮断するような検光子10の相対関係であれば
、人間の眼またはテレビカメラで見られる視野は完全暗
黒状態であり、また逆に反射後の偏光された光7等を通
過させるような検光子10の相対関係であれば、人間の
眼またはテレビカメラで見られる視野は完全明視野であ
る。By analyzing the PN junction region 1 from which the insulating film, metallization, etc. have been removed, it can be determined whether the leakage current is truly due to a defect in the PN junction. FIG. 1a shows a state in which the PN junction region 1 is exposed on the semiconductor substrate 2. In FIG.
In the analysis method according to the present invention, the exposed main surface 2a of the semiconductor substrate 2 in the PN junction region 1 is covered with a field effect crystal film 3 (FIG. 1b), and then the glass plate 4 is It is placed on the field effect type liquid crystal film 3. The coverage area of the field-effect liquid crystal film 3 and the shape and size of the glass plate 4 are set to a shape and size that can sufficiently cover the PN junction region 1 that is the object of analysis (FIG. 1c). Subsequently, as shown in FIG. 2, the sample 100 provided with the field effect liquid crystal film 3 and the glass plate 4 is placed under an optical system 200. The optical system 200 is for projecting light 7, which is obtained by polarizing light from the light source 5 using a polarizer 6, onto the PN junction region 1. Either the unpolarized normal light 7' from the light source 5'' is also projected onto the PN junction region 1, or this normal light 7'', unlike the optical path of the polarized light 7, is directly obliquely incident on the surface of the sample 100. P
The N-junction region 1 is irradiated, and the beam is uniformly reflected by the surface of the sample 100 and emitted. Therefore, the normal light 7'' does not pass through the eyepiece 11. On the other hand, the polarized light 7 passes through the prism 8.
, passes through the objective lens 9, the glass plate 4, and the field effect type liquid crystal film 3, reaches the PN junction region 1, and is reflected there. Then, the reflected light passes through the field effect liquid crystal film 3, the glass plate 4, and the objective lens 9 again and reaches the prism 8. The prism 8 is a semi-transparent mirror, and the reflected polarized light 7 travels straight, passes through an analyzer 10 and an eyepiece 11, and is observed by the human eye or a television camera. Objective lens 9, eyepiece lens 11
is provided to enlarge the minute PN junction region 1 for detailed observation. If the relative relationship between the polarizer 6 and the analyzer 10 in terms of the polarization plane is such that the analyzer 10 blocks the reflected polarized light 7, etc., then the field of view seen by the human eye or a television camera is If the analyzer 10 is in a completely dark state and the relative relationship of the analyzer 10 is such that it allows reflected polarized light 7, etc. to pass through, the field of view seen by the human eye or a television camera is a completely bright field.
ここでもし、電界効果型液晶膜3のある部分が複屈折を
起しているならば、複屈折を起している電界効果型液晶
膜3の部分を通過する偏光された光7等の偏波面に回転
が起り、検光子10を通じて観察される視野において、
暗黒状態の中に明るい視野、あるいは明視野の中に暗黒
部分が現われる。ところでPN接合に光か照射されると
光起電力を生じる現象のあることはよく知られている。Here, if a certain part of the field-effect liquid crystal film 3 has birefringence, the polarized light 7 etc. that passes through the part of the field-effect liquid crystal film 3 that has birefringence will be polarized. Rotation occurs in the wavefront, and in the field of view observed through the analyzer 10,
A bright field appears in a dark state, or a dark area appears within a bright field. By the way, it is well known that there is a phenomenon in which a photovoltaic force is generated when a PN junction is irradiated with light.
したがつて、偏光された光7等がPN接合領域1へ照射
された場合においてもPN接合領域1と半導体基板2の
間lこ光起電力を発生する。光起電力が誘起されればP
N接合領域1の半導体基板主面2aに現われているPN
接合線1aに亘つても電界か形成される。この電界は電
界効果型液晶膜3の中にも電気力線が通過するものであ
つて、電界効果型液晶膜3はこの電界によつて複屈折を
起す。この複屈折は偏光された光7等の偏波面を回転さ
せ、検光子10を通じて、人間の眼あるいはテレビカメ
ラで確認できることはすでに述べたとおりである。だか
もし、PN接合領域1のPN接合特性が不良であつて逆
方向リーク電流を引き起しているならば、偏光された光
7で誘起された光起電力は低下し、電界効果型液晶膜3
への電界は弱まり、検光子10を通じて観察される暗黒
状態の中での明視野の明るさ、または明視野中の暗黒部
分の暗らさは変化する。したかつて、PN接合特性のす
ぐれたPN接合領域とPN接合特性の良くないPN接合
領域の、比較観察によつてPN接合特性の良否を判定す
ることができる。第1図では図示していないが、集積回
路のごとき半導体素子では、数多くのPN接合領域が形
成されているので、良否判定を要するPN接合領域の周
辺には必ずいくつかの他のPN接合領域も存在している
から、この良否判定対象外のPN接合領域群と良否判定
対象のPN接合領域を比較することができ、これにより
PN接合特性の良否を判定できる。またPN接合リーク
電流によつて生じた解析対象のPN接合領域1に向けて
、偏光された光7の光路以外から、通常光を照射するよ
うにしたので、申+″!發=:(―呻=ないような完全
暗黒状態あるいは完全明視野となり、これによりPN接
合リーク電流が他の電気回路へ悪影響を及ぼす。Therefore, even when the PN junction region 1 is irradiated with polarized light 7 or the like, a photovoltaic force is generated between the PN junction region 1 and the semiconductor substrate 2. If a photovoltaic force is induced, P
PN appearing on the main surface 2a of the semiconductor substrate in the N junction region 1
An electric field is also formed across the bonding line 1a. This electric field causes electric lines of force to pass through the field effect liquid crystal film 3, and the field effect liquid crystal film 3 causes birefringence due to this electric field. As described above, this birefringence rotates the plane of polarization of the polarized light 7, etc., and can be confirmed by the human eye or a television camera through the analyzer 10. However, if the PN junction characteristics of the PN junction region 1 are poor and cause a reverse leakage current, the photoelectromotive force induced by the polarized light 7 decreases, and the field effect liquid crystal film 3
The electric field weakens, and the brightness of the bright field in the dark state or the darkness of the dark part in the bright field observed through the analyzer 10 changes. In the past, it was possible to determine whether the PN junction characteristics were good or bad by comparing and observing a PN junction region with excellent PN junction characteristics and a PN junction region with poor PN junction characteristics. Although not shown in FIG. 1, many PN junction regions are formed in a semiconductor device such as an integrated circuit, so there are always several other PN junction regions around the PN junction region that requires pass/fail determination. Since the PN junction region group that is not subject to quality determination can be compared with the PN junction region that is subject to quality determination, it is possible to determine the quality of the PN junction characteristics. In addition, normal light was irradiated from a path other than the optical path of the polarized light 7 toward the PN junction region 1 to be analyzed caused by the PN junction leakage current. This results in a completely dark state or a completely bright field, which causes the PN junction leakage current to adversely affect other electrical circuits.
即ち不良箇所が正常箇所をも不正常としてしまうの言防
止でき、PN接合の良否を正確に判定することができる
。また電解効果型液晶の種類によつては、比較的長時間
の光照射によつて、複屈折の度合が緩和されて、電界効
果型液晶膜3の光学的性質が電界依存性を示さない場合
があるが、本実施例ではこの場合には、偏光された光7
及び通常光のように偏光されていない光を断続光とした
ので上記液晶の電界効果が弱まることはなく、明確なP
N接合良否判定を行うことができる。In other words, it is possible to prevent a defective portion from turning a normal portion into an abnormal one, and it is possible to accurately determine the quality of the PN junction. Depending on the type of field-effect liquid crystal, the degree of birefringence may be alleviated by light irradiation for a relatively long period of time, and the optical properties of the field-effect liquid crystal film 3 may not show electric field dependence. However, in this example, in this case, the polarized light 7
And since the light that is not polarized like normal light is used as intermittent light, the electric field effect of the liquid crystal is not weakened, and a clear P
N-junction quality determination can be performed.
電界効果型液晶膜3には例えばMBBA(P−Meth
Oxybenzylidene−P−Butylani
line)などのネマチツク液晶を用いる。The field effect liquid crystal film 3 is made of, for example, MBBA (P-Meth).
Oxybenzylidene-P-Butylani
A nematic liquid crystal such as LINE) is used.
MBBAのごとき液晶の絶縁抵抗は1010Ω儂以上で
あつて、PN接合領域上へ直線塗布しても液晶によるり
ーク電流は非常に小さい。以上詳しく述べたように本発
明によるPN接合領域のPN接合特性の良否を判定でき
る不良解析法は、PN接合領域上に、電界効果型液晶膜
及びガラス板を設け、これらを通して上記PN接合領域
に偏光された光及び偏光されていない光を同時に重複し
てかつ断続的に投射したので、PN接合領域に何ら金属
電極を形成することなく、簡単な操作にもとづいて微細
パターンのPN接合領域を解析でき、この際にPN接合
リーク電流が他の電気回路に悪影響を与えることがなく
、また液晶の電解効果を弱めることのない効果がある。The insulation resistance of a liquid crystal such as MBBA is 1010 Ω or more, and the leakage current caused by the liquid crystal is very small even if it is applied linearly onto the PN junction region. As described in detail above, the failure analysis method according to the present invention that can determine the quality of the PN junction characteristics of the PN junction region is such that a field effect liquid crystal film and a glass plate are provided on the PN junction region, and the PN junction region is connected to the PN junction region through these. Since polarized light and unpolarized light are simultaneously projected overlappingly and intermittently, the PN junction region of a fine pattern can be analyzed based on simple operations without forming any metal electrodes in the PN junction region. In this case, the PN junction leakage current does not adversely affect other electric circuits, and the electrolytic effect of the liquid crystal is not weakened.
もしPN接合領域に局部的な暗黒部または輝点が見出さ
れるならば、単にPN接合領域そのものの良否判定だけ
にとどまらず不良個所をも発見できる。If a local dark area or bright spot is found in the PN junction region, it is possible not only to simply determine the quality of the PN junction region itself, but also to discover defective locations.
ますます高集積化され微細パターン化する集積回路等に
対する本発明の不良解析法の適用は、よりよいPN接合
形成の手掛り、改善をもたらすものであつて、ひいては
半導体素子製造技術の進歩を促すものである。Application of the failure analysis method of the present invention to integrated circuits, etc., which are becoming increasingly highly integrated and finely patterned, will provide clues and improvements to the formation of better PN junctions, and will further promote progress in semiconductor device manufacturing technology. It is.
第1図は本発明による半導体素子の不良解析法を適用す
るにあたつての試料処理法を説明するための工程別断面
図、第2図は本発明による不良解析法を適用するための
光学系の概要図を示す。
1はPN接合領域、2は半導体基板、3は電界効果型液
晶膜、4はガラス板、6は偏光子、7は偏光された光、
8はプリズム、9は対物レンズ、10は検光子、11は
接眼レンズ、100は試料、200は光学系である。FIG. 1 is a cross-sectional view of each step to explain a sample processing method when applying the failure analysis method for semiconductor devices according to the present invention, and FIG. 2 is an optical diagram for applying the failure analysis method according to the present invention. A schematic diagram of the system is shown. 1 is a PN junction region, 2 is a semiconductor substrate, 3 is a field effect liquid crystal film, 4 is a glass plate, 6 is a polarizer, 7 is polarized light,
8 is a prism, 9 is an objective lens, 10 is an analyzer, 11 is an eyepiece, 100 is a sample, and 200 is an optical system.
Claims (1)
純物が拡散されてなるPN接合領域のPN接合性の不良
解析法において、前記PN接合領域を充分に覆う電界効
果型液晶膜を前記PN接合領域上に形成し、さらに前記
PN接合領域を充分に覆うガラス板を前記電界効果型液
晶膜上に載置し、偏光された光と偏光されていない光と
を同時に重複してかつ断続的に前記ガラス板、前記電界
効果型液晶膜を通して前記PN接合領域に照射し、前記
PN接合領域、前記電解効果型液晶より反射された光を
検光子にて観察することを特徴とする半導体素子の不良
解析法。1. In a method for analyzing failure of PN junction in a PN junction region in which impurities of a conductivity type opposite to that of the semiconductor substrate are diffused into the main surface of a semiconductor substrate, a field effect liquid crystal film sufficiently covering the PN junction region is formed in the PN junction region. A glass plate is formed on the bonding region and further covers the PN junction region sufficiently, and is placed on the field effect liquid crystal film to simultaneously emit polarized light and unpolarized light in an overlapping and intermittent manner. irradiating the PN junction region through the glass plate and the field effect liquid crystal film, and observing the light reflected from the PN junction region and the field effect liquid crystal with an analyzer. Failure analysis method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP713477A JPS5921169B2 (en) | 1977-01-24 | 1977-01-24 | Failure analysis method for semiconductor devices |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP713477A JPS5921169B2 (en) | 1977-01-24 | 1977-01-24 | Failure analysis method for semiconductor devices |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5392672A JPS5392672A (en) | 1978-08-14 |
| JPS5921169B2 true JPS5921169B2 (en) | 1984-05-18 |
Family
ID=11657598
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP713477A Expired JPS5921169B2 (en) | 1977-01-24 | 1977-01-24 | Failure analysis method for semiconductor devices |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5921169B2 (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6342498U (en) * | 1986-09-05 | 1988-03-19 | ||
| JPS6385597U (en) * | 1986-11-26 | 1988-06-04 | ||
| JPH0219971U (en) * | 1988-07-15 | 1990-02-09 |
-
1977
- 1977-01-24 JP JP713477A patent/JPS5921169B2/en not_active Expired
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6342498U (en) * | 1986-09-05 | 1988-03-19 | ||
| JPS6385597U (en) * | 1986-11-26 | 1988-06-04 | ||
| JPH0219971U (en) * | 1988-07-15 | 1990-02-09 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5392672A (en) | 1978-08-14 |
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