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JPS6130739B2 - - Google Patents
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JPS6130739B2 - - Google Patents

Info

Publication number
JPS6130739B2
JPS6130739B2 JP54090195A JP9019579A JPS6130739B2 JP S6130739 B2 JPS6130739 B2 JP S6130739B2 JP 54090195 A JP54090195 A JP 54090195A JP 9019579 A JP9019579 A JP 9019579A JP S6130739 B2 JPS6130739 B2 JP S6130739B2
Authority
JP
Japan
Prior art keywords
region
conductivity type
impurity region
high concentration
semiconductor substrate
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
JP54090195A
Other languages
Japanese (ja)
Other versions
JPS5613741A (en
Inventor
Kyoto Watari
Takeshi Fukuda
Tadashi Kirisako
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 JP9019579A priority Critical patent/JPS5613741A/en
Publication of JPS5613741A publication Critical patent/JPS5613741A/en
Publication of JPS6130739B2 publication Critical patent/JPS6130739B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10PGENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
    • H10P74/00Testing or measuring during manufacture or treatment of wafers, substrates or devices

Landscapes

  • Testing Or Measuring Of Semiconductors Or The Like (AREA)

Description

【発明の詳細な説明】 本発明は半導体装置、特に半導体ウエーハを拡
散工程中にサンプリングして検査するプロービン
グテスト用のモニタ・パターンを備えた半導体装
置に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a semiconductor device, and more particularly to a semiconductor device equipped with a monitor pattern for a probing test in which a semiconductor wafer is sampled and inspected during a diffusion process.

半導体ウエーハに多数の半導体集積回路素子を
形成する場合に、個々の素子の一偶にモニタ・パ
ターンを形成し、該モニタ・パターンによつてト
ランジスタ素子特性などを検査して不純物拡散層
の深さや濃度を工程途中で制御する方法が用いら
れる、 該検査方法はベース領域などに探針を接触させ
て測定するプロービングテストと呼ばれるが、一
枚のウエーハに形成される素子数が多いために、
時間の浪費を避け、またウエーハ内の位置による
バラツキをも知るために、手動によるサンプリン
グが通常行われており、量産工程にあつては歩留
を保持するために極めて重要なテストであると共
に、微細な調整を必要とするために多くの工数を
要する工程である。
When forming a large number of semiconductor integrated circuit elements on a semiconductor wafer, a monitor pattern is formed on each element, and transistor element characteristics are inspected using the monitor pattern to determine the depth of the impurity diffusion layer and the like. A method of controlling the concentration during the process is used. This inspection method is called a probing test, in which a probe is brought into contact with the base region, etc., but since the number of elements formed on one wafer is large,
Manual sampling is usually performed to avoid wasting time and to find out variations due to position within the wafer, and is an extremely important test to maintain yield in mass production processes. This is a process that requires many man-hours because it requires minute adjustments.

このようなプロビングテストで測定するトラン
ジスタ素子特性の内、特に重要なのは電流増巾率
(hFE)であり、安定した製作工程では例えば第
1図a及びbに示すような横巾250μm、縦巾130
μm程度のモニタ・パターンを形成して、電流増
巾率(hFE)のみを推定する測定方法が用いられ
ている。
Of the transistor device characteristics measured in such probing tests, the particularly important one is the current amplification factor (h FE ), and in a stable manufacturing process, Width 130
A measurement method is used in which a monitor pattern on the order of μm is formed and only the current amplification factor (h FE ) is estimated.

第1図aは平面図で、第1図bは第1図aの
AA′断面図を示しており、npn型素子の場合には
n型エピタキシヤル層1内に、P+型ベース領域
2を形成せしめ、該ベース領域2を横切つてn+
型エミツタ領域3を形成せしめている。そして、
ベース領域2の両側領域の中心位置2′及び2″に
それぞれ探針を接触せしめて、両探針間に数Vの
電圧を印加し、電流を流すと第1図bに示してい
るエミツタ領域3の下部のベース領域の厚み4に
逆比例した抵抗があらわれる。これをピンチ抵抗
と称しているが、このようなピンチ抵抗は通常数
KΩから数十KΩで、高抵抗があらわれると高い
FEのトランジスタが形成されていることにな
り、このピンチ抵抗を測定して、hFEを推定し拡
散工程の制御を行なう。
Figure 1a is a plan view, and Figure 1b is the same as Figure 1a.
In the case of an npn type device, a p + type base region 2 is formed in an n type epitaxial layer 1, and an n + type base region 2 is formed across the base region 2 .
A mold emitter region 3 is formed. and,
When probes are brought into contact with the central positions 2' and 2'' of both sides of the base region 2, a voltage of several volts is applied between both probes, and a current is caused to flow, the emitter region shown in Fig. 1b is formed. A resistance appears that is inversely proportional to the thickness 4 of the base region at the bottom of 3. This is called a pinch resistance, and such a pinch resistance is usually from several KΩ to several tens of KΩ, and when a high resistance appears, a high h FE The pinch resistance is measured to estimate h FE and control the diffusion process.

しかしながらこのように2本の探針を近接して
接触させるには、探針の線径に限界があり、強い
接触圧力を加えることは難かしく、そのために表
面で接触抵抗が生じて正確なピンチ抵抗値を得る
ことができない問題がある。
However, in order to bring two probes into close contact in this way, there is a limit to the wire diameter of the probe, and it is difficult to apply strong contact pressure.As a result, contact resistance occurs on the surface, making it difficult to accurately pinch. There is a problem that the resistance value cannot be obtained.

そうすれば誤つたhFEを推定することになり所
期の特性の半導体素子に制御することが難かしく
なる。
In this case, h FE will be estimated incorrectly, making it difficult to control the semiconductor element to have the desired characteristics.

本発明はこのような問題点を除去して、正確な
ピンチ抵抗値を得ることを目的として、一導電型
の半導体基板と、該半導体基板上に形成された反
対導電型のエピタキシヤル層と、該エピタキシヤ
ル層に形成された該半導体基板に達する第1の一
導電型高濃度不純物領域と、該エピタキシヤル層
に形成され該半導体基板に達しない第2の一導電
型高濃度不純物領域と、該第1および第2の高濃
度不純物領域に接続される一導電型の不純物領域
と、該不純物領域を横断し、かつ該不純物領域よ
り浅く形成された反対導電型の不純物領域を有す
るモニタパターンを具備することを特徴とする。
In order to eliminate such problems and obtain an accurate pinch resistance value, the present invention includes a semiconductor substrate of one conductivity type, an epitaxial layer of an opposite conductivity type formed on the semiconductor substrate, a first high concentration impurity region of one conductivity type formed in the epitaxial layer and reaching the semiconductor substrate; a second high concentration impurity region of one conductivity type formed in the epitaxial layer and not reaching the semiconductor substrate; a monitor pattern having an impurity region of one conductivity type connected to the first and second high concentration impurity regions, and an impurity region of the opposite conductivity type formed to cross the impurity region and to be shallower than the impurity region; It is characterized by comprising:

以下、本発明を一実施例によつて詳細に説明す
る。
Hereinafter, the present invention will be explained in detail by way of an example.

第2図a及びbはウエーハ内の個々の集積回路
素子に形成された本発明のモニタパターンの1パ
ターンの一実施例で、第2図aは平面図で、第2
図bは第2図aのBB′断面図である。
2a and 2b show one embodiment of the monitor pattern of the present invention formed on individual integrated circuit elements within a wafer; FIG. 2a is a plan view;
Figure b is a sectional view BB' of Figure 2a.

図において、P型半導体基板10にn+型埋込
拡散層12を拡散形成した後、該基板上にn型エ
ピタキシヤル層11を積層し、次いでp+型素子
分離領域13を形成する。その際に同時にP+
高濃度領域14をも拡散形成する。
In the figure, after an n + type buried diffusion layer 12 is diffused into a P type semiconductor substrate 10, an n type epitaxial layer 11 is laminated on the substrate, and then a p + type element isolation region 13 is formed. At the same time, the P + type high concentration region 14 is also formed by diffusion.

次いでP型ベース領域15を拡散形成するが、
該ベース領域15は一端が素子分離領域13と接
続し、他端は上記の高濃度領域14を包含したパ
ターン領域となつている。
Next, the P type base region 15 is formed by diffusion.
One end of the base region 15 is connected to the element isolation region 13, and the other end is a pattern region including the above-mentioned high concentration region 14.

次いでn+型エミツタ領域16をベース領域の
中央部分にベース領域を横断して形成せしめる。
Next, an n + type emitter region 16 is formed at the center of the base region and across the base region.

これらはすべて公知のフオトリソグラフイ技術
と拡散技術とを用いて集積回路素子と同時に形成
されるものである。
All of these are formed simultaneously with the integrated circuit elements using known photolithography and diffusion techniques.

モニタパターンをこのような構造に形成せしめ
ると、ピンチ抵抗は第2図bに示しているエミツ
タ領域16の下部のベース領域の厚み17に逆比
例した値となるが、一端は高濃度の素子分離領域
Bと接続しているので、探針を用いずに、半導体
基板の裏面より測定端子を取ることができる。
When the monitor pattern is formed in such a structure, the pinch resistance becomes inversely proportional to the thickness 17 of the base region below the emitter region 16 shown in FIG. Since it is connected to region B, the measurement terminal can be taken from the back surface of the semiconductor substrate without using a probe.

そして他端には探針を接触せしめるのであるが
該接触部分はP+型高濃度領域14と重複して拡
散形成している位置15′であり、非常に高濃度
となつているので、表面抵抗も低く、又その位置
にたゞ1本の探針のみを接触せしめるのであるか
ら線径が太くて強い探針を強く圧着して、接触抵
抗を大巾に減少せしめ得るので、正確なピンチ抵
抗値を測定することができて、従つて実際値によ
く一致したhFEを知ることができる。
The probe is brought into contact with the other end, but the contact portion is at a position 15' which overlaps with the P + type high concentration region 14 and is formed by diffusion, and has a very high concentration, so the surface The resistance is also low, and since only one probe is brought into contact with that position, a strong probe with a thick wire diameter can be strongly crimped and the contact resistance can be greatly reduced, allowing for accurate pinching. It is possible to measure the resistance value and thus to know h FE which closely corresponds to the actual value.

又、プロービングテストには1本の探針のみの
接触圧着操作でよいので、測定が容易で工数の減
少となり、自動的に測定させることも困難ではな
い。
In addition, since the probing test requires only one probe to be contacted and pressed, the measurement is easy and the number of man-hours is reduced, and it is not difficult to perform the measurement automatically.

以上、説明したように本発明は実際の集積回路
素子によく一致したhFEを知ることができるため
に、工程途中のトランジスタ特性の制御が容易に
なり、高品質の半導体装置の形成に役立ち、しか
も作業工数を減少させる効果もあり、極めて価値
高いものと言える。尚、上記説明ではnpn型半導
体素子を用いたが、npn型素子に適用できること
は当然である。
As described above, since the present invention can determine h FE that closely matches the actual integrated circuit element, it becomes easy to control transistor characteristics during the process, which is useful for forming high-quality semiconductor devices. Moreover, it has the effect of reducing the number of work hours, and can be said to be extremely valuable. Incidentally, in the above description, an npn type semiconductor element was used, but it goes without saying that the present invention can be applied to an npn type element.

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

第1図a及びbは従来のモニタパターン、第2
図a及びbは本発明のモニタパターンのそれぞれ
平面図及び断面図を示している。 図中、13は素子分離領域、14は同時に形成
される高濃度領域、15はベース領域、16はエ
ミツタ領域である。
Figures 1a and b are conventional monitor patterns;
Figures a and b show a plan view and a cross-sectional view, respectively, of a monitor pattern of the present invention. In the figure, 13 is an element isolation region, 14 is a high concentration region formed at the same time, 15 is a base region, and 16 is an emitter region.

Claims (1)

【特許請求の範囲】[Claims] 1 一導電型の半導体基板と、該半導体基板上に
形成された反対導電型のエピタキシヤル層と、該
エピタキシヤル層に形成され、該半導体基板に達
する第1の一導電型高濃度不純物領域と、該エピ
タキシヤル層に形成され該半導体基板に達しない
第2の一導電型高濃度不純物領域と、該第1およ
び第2の高濃度不純物領域に接続される一導電型
の不純物領域と、該不純物領域を横断し、かつ該
不純物領域より浅く形成された反対導電型の不純
物領域を有するモニタパターンを具備することを
特徴とする半導体装置。
1 A semiconductor substrate of one conductivity type, an epitaxial layer of an opposite conductivity type formed on the semiconductor substrate, and a first high concentration impurity region of one conductivity type formed in the epitaxial layer and reaching the semiconductor substrate. , a second high concentration impurity region of one conductivity type formed in the epitaxial layer and not reaching the semiconductor substrate; an impurity region of one conductivity type connected to the first and second high concentration impurity regions; 1. A semiconductor device comprising a monitor pattern having an impurity region of an opposite conductivity type formed to cross an impurity region and to be shallower than the impurity region.
JP9019579A 1979-07-16 1979-07-16 Semiconductor device Granted JPS5613741A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9019579A JPS5613741A (en) 1979-07-16 1979-07-16 Semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9019579A JPS5613741A (en) 1979-07-16 1979-07-16 Semiconductor device

Publications (2)

Publication Number Publication Date
JPS5613741A JPS5613741A (en) 1981-02-10
JPS6130739B2 true JPS6130739B2 (en) 1986-07-15

Family

ID=13991692

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9019579A Granted JPS5613741A (en) 1979-07-16 1979-07-16 Semiconductor device

Country Status (1)

Country Link
JP (1) JPS5613741A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6121176A (en) * 1984-07-09 1986-01-29 Tatsuta Electric Wire & Cable Co Ltd Antifreeze composition

Also Published As

Publication number Publication date
JPS5613741A (en) 1981-02-10

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