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JP3661334B2 - Minority carrier lifetime measurement method and semiconductor device manufacturing method - Google Patents
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JP3661334B2 - Minority carrier lifetime measurement method and semiconductor device manufacturing method - Google Patents

Minority carrier lifetime measurement method and semiconductor device manufacturing method Download PDF

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Publication number
JP3661334B2
JP3661334B2 JP03015697A JP3015697A JP3661334B2 JP 3661334 B2 JP3661334 B2 JP 3661334B2 JP 03015697 A JP03015697 A JP 03015697A JP 3015697 A JP3015697 A JP 3015697A JP 3661334 B2 JP3661334 B2 JP 3661334B2
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Japan
Prior art keywords
layer
lifetime
soi
charge
pad electrode
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JP03015697A
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JPH10229109A (en
Inventor
成生 佐藤
義春 戸坂
博幸 金田
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Fujitsu Ltd
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Fujitsu Ltd
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Description

【0001】
【発明の属する技術分野】
本発明は半導体装置における少数キャリアのライフタイムの測定技術に係り、特に絶縁膜上に単結晶シリコン層を積層させてなるSOI構造の半導体装置における少数キャリアのライフタイムの測定法に関するものである。
【0002】
Silicon on Insulator構造(以下、SOI構造と略称する)のMOSFETは寄生容量が少ないことが特徴であるから消費電力が少なく、また、DRAMに適用すると、ピット線容量が少なくなり、高速で動作させることが可能である。
【0003】
しかし、SOI構造には、埋め込み酸化膜とシリコン界面の少数キャリアのライフタイムが短いという問題がある。ライフタイムが短いと、pn接合の逆方向リーク電流が大きくなり、消費電力の増加や、DRAMの電荷保持特性の劣化などの問題が生じる。
【0004】
このため、SOI構造では、少数キャリアのライフタイムを定量的にモニターすることが必要である。
以上のような状況から、SOI層の少数キャリアのライフタイムを正確に測定することが可能な少数キャリアのライフタイムの測定法が要望されている。
【0005】
【従来の技術】
従来のSOI層内に発生させた少数キャリアが再結合して消滅するまでの時間、即ち少数キャリアのライフタイムの測定は、一般に、SOI層に波長が 800nm〜1,000nm の電磁波を照射して少数キャリアを励起し、この少数キャリアの濃度の経時変化を、SOI層に照射したマイクロ波の反射強度を計測することにより行われている。
【0006】
このようなマイクロ波を用いる少数キャリア濃度の測定については、例えば、 "Microwave Techniques in Measurement of Lifetime in Germanium",Journal of Applied Physics,Vol.30,N0.7,pp.1054-1060(1959) に記載されている。
【0007】
【発明が解決しようとする課題】
以上説明した従来の少数キャリアのライフタイムの測定法においては、可視光をSOI層に照射すると、数十μm 程度の深さまで可視光が到達することが知られている。
【0008】
SOI層に可視光を照射した場合には、可視光がSOI層の支持基板に達し、この支持基板部分においても少数キャリアが励起されるため、SOI層にのみ励起された少数キャリアのライフタイムを正確に測定することができないという課題があった。
【0009】
本発明は以上のような状況から、簡単且つ容易にSOI層のみに励起された少数キャリアのライフタイムの測定を行うことが可能となる少数キャリアのライフタイムの測定法の提供を目的としたものである。
【0010】
【課題を解決するための手段】
本発明の少数キャリアのライフタイムの測定法は、p型のSOI層にp+層とn+層を形成し、このp+層とn+層とをそれぞれp+層パッド電極とn+パッド層電極と接続するメタル配線層を備えた半導体装置における少数キャリアのライフタイムの測定法において、このn+層パッド電極とアースの間に電荷計測器を設け、このp+層パッド電極をアースに接続し、このp+層とn+層との間のSOI層にイオンを注入した際にこの電荷計測器によりこのn+層パッド電極に収集された電荷量を計測し、このイオンの注入位置と収集電荷量の関係に基づき、このSOI層の少数キャリアのライフタイムを算出するように構成する。
【0011】
即ち本発明においては図1に示すように、支持基板1の表面に絶縁膜2を形成し、この絶縁膜2の表面にp層からなるSOI層3を形成し、このSOI層3の表面にp+層4とn+層5を形成し、n+層5とアースの間に電荷計測器8を設けて、このp+層4とn+層5との間のSOI層3にイオン7を注入すると、SOI層3内及び支持基板1内に少数キャリアが励起されるが、SOI層3と支持基板1との間に絶縁膜2が形成されているので、支持基板1に励起された少数キャリアは、この電荷計測器8の測定には影響を与えず、SOI層3のみに励起された少数キャリアのライフタイムの測定を行うことが可能となる。
【0012】
この場合、イオンの照射位置と拡散層、即ちn+層との距離と、この電荷計測器により収集した収集電荷量との関係は図2に示すようになり、この距離が大きくなればこの収集電荷量が減少するので、入射位置に対応する収集電荷量を測定し、図2において入射位置の線と収集電荷量の線との交点でライフタイムを見つけることにより、SOI層3の少数キャリアのライフタイムの測定を行うことが可能となる。
【0013】
【発明の実施の形態】
以下図3〜図9により本発明の第1〜第4の実施例について詳細に説明する。
図3は本発明による第1の実施例の断面図、図4は本発明による第1の実施例の平面図、図5は本発明による第2の実施例の断面図、図6は本発明による第2の実施例の平面図、図7は本発明による第3の実施例の断面図、図8は本発明による第3の実施例の平面図、図9は本発明による第4の実施例の断面図である。
【0014】
本発明による第1の実施例においては、図3に示すようにp型シリコン層13に50μm の間隔でp+層4とn+層5を形成し、図4に示すようにp+層4とp+層パッド電極4aとをアルミニウムなどからなるメタル配線6aで接続し、n+層5とn+層パッド電極5aとをアルミニウムなどからなるメタル配線6bで接続する。
【0015】
そして、0.1 fCの精度で電荷を計測することが可能な電荷計測器8をn+層パッド電極を介して図1に示すようにこのn+層5に接続する。
その後、図3に示すようにこのn+層5とp+層4の間に数MeV程度に加速したイオン7を照射し、この電荷計測器8により収集電荷量を計測する。
【0016】
イオンの照射位置の制御は、平行平板型のコンデンサにより数μm の精度で行うことが必要である。
そして、図2を用いて、イオンの入射位置の線と収集電荷量の線との交点でライフタイムを見つけることにより、SOI層3の少数キャリアのライフタイムの測定を行うことが可能となる。
【0017】
本発明による第2の実施例においては、図5に示すようにp型シリコン層13に50μm の間隔でp+層4とn+層5を形成し、図6に示すようにp+層4とp+層パッド電極4aとをアルミニウムなどからなるメタル配線6aで接続し、n+層5とn+層パッド電極5aとをアルミニウムなどからなるメタル配線6bで接続する。
【0018】
そして、0.1 fCの精度で電荷を計測することが可能な電荷計測器8をn+層パッド電極を介して図1に示すようにこのn+層5に接続する。
この第2の実施例においては、メタル配線6a,6b を形成した後、図5に示すようにα線を遮蔽することができる膜厚30μm のポリイミド膜9を堆積し、このポリイミド膜9に図6に示すように2μm □のポリイミドホール9aを形成する。
【0019】
そして、α線7bを放射するα線源7aをシリコン基板上に置くと、α線源7aから放射されるα線7bのエネルギーは約5MeVであるから、膜厚30μm のポリイミド膜9中でエネルギーが減衰し、p型シリコン層13までは到達しない。このためポリイミドホール9aの部分のみにα線7bが入射する。
【0020】
このポリイミドホール9aの位置と収集電荷量の関係から、第1の実施例の場合と同様に、少数キャリアのライフタイムの測定を行うことが可能となる。
この第2の実施例においては、α線7bの入射位置を決めるポリイミドホール9aをリソグラフィー技術を用いて形成するので、α線7bの入射位置の制御を安価に且つ簡単に行うことが可能である。
【0021】
本発明による第3の実施例においては、図7に示すようにp型シリコン層13に50μm の間隔でp+層4とn+層5を形成する前に、p型シリコン層13の表面にゲート酸化膜10b を介してゲート電極10を形成し、図8に示すようにp+層4とp+層パッド電極4aとをアルミニウムなどからなるメタル配線6aで接続し、n+層5とn+層パッド電極5aとをアルミニウムなどからなるメタル配線6bで接続する。
【0022】
そして、0.1 fCの精度で電荷を計測することが可能な電荷計測器8をn+層パッド電極を介して図1に示すようにこのn+層5に接続する。
この第3の実施例においては、電荷計測器8により電荷量を収集する際には、ゲート電極10に正の電圧を印加するから、p型シリコン層13に発生した電子は、ゲート電極10の直下の界面を流れるようになるので、第1の実施例や第2の実施例においてはp型シリコン層13の上側の界面と下側の界面のライフタイムを別々に測定出来なかったが、この第3の実施例ではp型シリコン層13の上側の界面のライフタイムの測定を行うことが可能となる。
【0023】
本発明による第4の実施例においては、図9に示すように酸化膜12の形成工程中にゲート電極10を形成した後、ゲート酸化膜10b を介してp型シリコン層13を形成し、50μm の間隔でp+層4とn+層5を形成し、0.1 fCの精度で電荷を計測することが可能な電荷計測器8をn+層パッド電極を介して図1に示すようにこのn+層5に接続する。
【0024】
その後、図9に示すようにこのn+層5とp+層4の間に数MeV程度に加速したイオン7を照射し、この電荷計測器8により収集電荷量を計測する。
【0025】
イオンの照射位置の制御は、平行平板型のコンデンサにより数μm の精度で行うことが必要である。
この第4の実施例においても第3の実施例と同様に、電荷計測器8により電荷量を収集する際には、ゲート電極10に正の電圧を印加するから、p型シリコン層13に発生した電子は、この場合はゲート電極10の直上の界面を流れるようになるので、第1の実施例や第2の実施例においてはp型シリコン層13の上側の界面と下側の界面のライフタイムを別々に測定出来なかったが、この第4の実施例ではp型シリコン層13の下側の界面のライフタイムの測定を行うことが可能となる。
【0026】
本実施例では、n+層パッド電極とアースの間に電荷計測器を設け、p+層パッド電極をアースに接続し、このp+層とn+層との間のSOI層にイオンを注入した際にこの電荷計測器によりこのn+層パッド電極に収集された電荷量を計測し、このイオンの注入位置と収集電荷量の関係に基づき、このSOI層の少数キャリアのライフタイムを算出しているが、本実施例とは逆に電荷計測器をp+層パッド電極とアースの間に設け、n+層パッド電極をアースに接続し、このn+層とp+層との間のSOI層にイオンを注入した際にこの電荷計測器によりこのp+層パッド電極に収集された電荷量を計測し、このイオンの注入位置と収集電荷量の関係に基づき、このSOI層の正孔の少数キャリアのライフタイムを算出することが可能となる。
【0027】
【発明の効果】
以上の説明から明らかなように、本発明によれば極めて簡単な方法により支持基板の表面のSOI層に形成した少数キャリアのライフタイムの測定を、半導体装置の製造工程の途中において行うことが可能で、少数キャリアのライフタイムの短い半導体基板を工程の途中で除去することができる利点があり、著しい経済的及び、信頼性向上の効果が期待できる少数キャリアのライフタイムの測定法及び半導体装置の製造方法の提供が可能である。
【図面の簡単な説明】
【図1】 本発明の原理図
【図2】 n+層とイオン入射位置との距離と電荷計測器により収集した収集電荷量との関係を示す図
【図3】 本発明による第1の実施例の断面図
【図4】 本発明による第1の実施例の平面図
【図5】 本発明による第2の実施例の断面図
【図6】 本発明による第2の実施例の平面図
【図7】 本発明による第3の実施例の断面図
【図8】 本発明による第3の実施例の平面図
【図9】 本発明による第4の実施例の断面図
【符号の説明】
1 支持基板
2 絶縁膜
3 SOI層
4 p+
4a p+層パッド電極
5 n+
5a n+層パッド電極
6a メタル配線
6b メタル配線
7 イオン
7a α線源
7b α線
8 電荷計測器
9 ポリイミド膜
9a ポリイミドホール
10 ゲート電極
10a ゲート電極のパッド電極
10b ゲート酸化膜
11 シリコン基板
12 酸化膜
13 p型シリコン層
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a technique for measuring the lifetime of minority carriers in a semiconductor device, and more particularly to a method for measuring the lifetime of minority carriers in a semiconductor device having an SOI structure in which a single crystal silicon layer is stacked on an insulating film.
[0002]
A MOSFET with a silicon on insulator structure (hereinafter abbreviated as SOI structure) is characterized by low parasitic capacitance, and therefore consumes less power. When applied to a DRAM, the pit line capacitance is reduced and the MOSFET operates at high speed. Is possible.
[0003]
However, the SOI structure has a problem that the lifetime of minority carriers at the buried oxide film and the silicon interface is short. If the lifetime is short, the reverse leakage current of the pn junction becomes large, causing problems such as an increase in power consumption and deterioration in charge retention characteristics of the DRAM.
[0004]
For this reason, in the SOI structure, it is necessary to quantitatively monitor the lifetime of minority carriers.
Under the circumstances as described above, there is a demand for a method for measuring the lifetime of minority carriers capable of accurately measuring the lifetime of minority carriers in the SOI layer.
[0005]
[Prior art]
The time until the minority carriers generated in the conventional SOI layer recombine and disappear, that is, the minority carrier lifetime, is generally measured by irradiating the SOI layer with an electromagnetic wave having a wavelength of 800 nm to 1,000 nm. The time-dependent change of the minority carrier concentration is performed by exciting the carriers and measuring the reflection intensity of the microwave irradiated to the SOI layer.
[0006]
For the measurement of minority carrier concentration using such microwaves, see, for example, “Microwave Techniques in Measurement of Lifetime in Germanium”, Journal of Applied Physics, Vol. 30, N0.7, pp. 1054-1060 (1959). Has been described.
[0007]
[Problems to be solved by the invention]
In the conventional minority carrier lifetime measurement method described above, it is known that visible light reaches a depth of about several tens of μm when visible light is irradiated onto the SOI layer.
[0008]
When the SOI layer is irradiated with visible light, the visible light reaches the support substrate of the SOI layer, and minority carriers are excited also in this support substrate portion. Therefore, the lifetime of the minority carriers excited only in the SOI layer is reduced. There was a problem that it could not be measured accurately.
[0009]
The present invention aims to provide a method for measuring the lifetime of minority carriers that makes it possible to easily and easily measure the lifetime of minority carriers excited only in the SOI layer from the above situation. It is.
[0010]
[Means for Solving the Problems]
Measurement of the minority carrier lifetime of the present invention, p-type a p + layer and the n + layer was formed on the SOI layer, the p + layer and the n + layer and the respective p + layer pad electrode and the n + pad In a method for measuring the minority carrier lifetime in a semiconductor device having a metal wiring layer connected to a layer electrode, a charge measuring device is provided between the n + layer pad electrode and the ground, and the p + layer pad electrode is connected to the ground. When the ions are implanted into the SOI layer between the p + layer and the n + layer, the amount of charge collected in the n + layer pad electrode is measured by the charge measuring device, and the ion implantation position is measured. The lifetime of minority carriers in the SOI layer is calculated based on the relationship between the collected charge amount and the SOI layer.
[0011]
That is, in the present invention, as shown in FIG. 1, an insulating film 2 is formed on the surface of the support substrate 1, an SOI layer 3 composed of a p layer is formed on the surface of the insulating film 2, and the surface of the SOI layer 3 is formed. A p + layer 4 and an n + layer 5 are formed, a charge measuring device 8 is provided between the n + layer 5 and the ground, and ions 7 are formed in the SOI layer 3 between the p + layer 4 and the n + layer 5. Is injected into the SOI layer 3 and the support substrate 1, but since the insulating film 2 is formed between the SOI layer 3 and the support substrate 1, the minority carriers are excited by the support substrate 1. Minority carriers do not affect the measurement of the charge measuring device 8, and the lifetime of minority carriers excited only in the SOI layer 3 can be measured.
[0012]
In this case, the relationship between the distance between the ion irradiation position and the diffusion layer, that is, the n + layer, and the collected charge amount collected by the charge measuring device is as shown in FIG. Since the charge amount decreases, the collected charge amount corresponding to the incident position is measured, and the lifetime is found at the intersection of the incident position line and the collected charge amount line in FIG. Lifetime can be measured.
[0013]
DETAILED DESCRIPTION OF THE INVENTION
Hereinafter, the first to fourth embodiments of the present invention will be described in detail with reference to FIGS.
3 is a sectional view of the first embodiment of the present invention, FIG. 4 is a plan view of the first embodiment of the present invention, FIG. 5 is a sectional view of the second embodiment of the present invention, and FIG. 6 is the present invention. FIG. 7 is a sectional view of a third embodiment according to the present invention, FIG. 8 is a plan view of the third embodiment according to the present invention, and FIG. 9 is a fourth embodiment according to the present invention. It is sectional drawing of an example.
[0014]
In the first embodiment according to the present invention, to form a p + layer 4 and n + layer 5 at intervals of 50μm to p-type silicon layer 13 as shown in FIG. 3, p + layer 4 as shown in FIG. 4 And p + layer pad electrode 4a are connected by metal wiring 6a made of aluminum or the like, and n + layer 5 and n + layer pad electrode 5a are connected by metal wiring 6b made of aluminum or the like.
[0015]
Then, a charge measuring device 8 capable of measuring charges with an accuracy of 0.1 fC is connected to the n + layer 5 through an n + layer pad electrode as shown in FIG.
Thereafter, as shown in FIG. 3, ions 7 accelerated to about several MeV are irradiated between the n + layer 5 and the p + layer 4, and the collected charge amount is measured by the charge measuring device 8.
[0016]
The ion irradiation position needs to be controlled with a precision of several μm using a parallel plate capacitor.
Then, by using FIG. 2, the lifetime of minority carriers in the SOI layer 3 can be measured by finding the lifetime at the intersection of the ion incident position line and the collected charge amount line.
[0017]
In the second embodiment according to the present invention, to form a p + layer 4 and n + layer 5 at intervals of 50μm to p-type silicon layer 13 as shown in FIG. 5, p + layer 4 as shown in FIG. 6 And p + layer pad electrode 4a are connected by metal wiring 6a made of aluminum or the like, and n + layer 5 and n + layer pad electrode 5a are connected by metal wiring 6b made of aluminum or the like.
[0018]
Then, a charge measuring device 8 capable of measuring charges with an accuracy of 0.1 fC is connected to the n + layer 5 through an n + layer pad electrode as shown in FIG.
In the second embodiment, after forming the metal wirings 6a and 6b, a polyimide film 9 having a film thickness of 30 μm capable of shielding α rays is deposited as shown in FIG. As shown in FIG. 6, a 2 μm square polyimide hole 9a is formed.
[0019]
When the α-ray source 7a that emits the α-ray 7b is placed on the silicon substrate, the energy of the α-ray 7b emitted from the α-ray source 7a is about 5 MeV. Attenuates and does not reach the p-type silicon layer 13. For this reason, α rays 7b are incident only on the polyimide hole 9a.
[0020]
From the relationship between the position of the polyimide hole 9a and the collected charge amount, it is possible to measure the minority carrier lifetime as in the first embodiment.
In the second embodiment, since the polyimide hole 9a for determining the incident position of the α-ray 7b is formed using the lithography technique, it is possible to control the incident position of the α-ray 7b inexpensively and easily. .
[0021]
In the third embodiment according to the present invention, before the p + layer 4 and the n + layer 5 are formed on the p type silicon layer 13 at an interval of 50 μm as shown in FIG. forming a gate electrode 10 through the gate oxide film 10b, and a p + layer 4 and the p + layer pad electrode 4a as shown in FIG. 8 are connected by metal wiring 6a made of aluminum, n + layer 5 and the n The + layer pad electrode 5a is connected by a metal wiring 6b made of aluminum or the like.
[0022]
Then, a charge measuring device 8 capable of measuring charges with an accuracy of 0.1 fC is connected to the n + layer 5 through an n + layer pad electrode as shown in FIG.
In the third embodiment, when a charge amount is collected by the charge measuring device 8, a positive voltage is applied to the gate electrode 10. Therefore, electrons generated in the p-type silicon layer 13 Since it flows through the interface immediately below, the lifetimes of the upper interface and the lower interface of the p-type silicon layer 13 could not be measured separately in the first and second embodiments. In the third embodiment, the lifetime of the upper interface of the p-type silicon layer 13 can be measured.
[0023]
In the fourth embodiment according to the present invention, as shown in FIG. 9, after forming the gate electrode 10 during the step of forming the oxide film 12, the p-type silicon layer 13 is formed via the gate oxide film 10b, and 50 .mu.m. the n of the p + layer 4 and n + layer 5 were formed at intervals, 0.1 fC of the charge measuring instrument 8 capable of measuring charges in precision as shown in FIG. 1 via the n + layer pad electrode + Connect to layer 5.
[0024]
Thereafter, as shown in FIG. 9, ions 7 accelerated to about several MeV are irradiated between the n + layer 5 and the p + layer 4, and the collected charge amount is measured by the charge measuring device 8.
[0025]
The ion irradiation position needs to be controlled with a precision of several μm using a parallel plate capacitor.
In the fourth embodiment, as in the third embodiment, when a charge amount is collected by the charge measuring device 8, a positive voltage is applied to the gate electrode 10, so that it is generated in the p-type silicon layer 13. In this case, the electrons that have flown flow through the interface immediately above the gate electrode 10, so that the life of the upper interface and the lower interface of the p-type silicon layer 13 is reduced in the first and second embodiments. Although the time could not be measured separately, in the fourth embodiment, the lifetime of the lower interface of the p-type silicon layer 13 can be measured.
[0026]
In this embodiment, a charge measuring device is provided between the n + layer pad electrode and the ground, the p + layer pad electrode is connected to the ground, and ions are implanted into the SOI layer between the p + layer and the n + layer. The charge amount collected by the n + layer pad electrode is measured by this charge measuring instrument and the lifetime of minority carriers in this SOI layer is calculated based on the relationship between the ion implantation position and the collected charge amount. However, contrary to the present embodiment, a charge measuring device is provided between the p + layer pad electrode and the ground, the n + layer pad electrode is connected to the ground, and the n + layer and the p + layer are connected to each other. When the ions are implanted into the SOI layer, the charge amount collected by the p + layer pad electrode is measured by the charge measuring device. Based on the relationship between the ion implantation position and the collected charge amount, the holes of the SOI layer are measured. It is possible to calculate the lifetime of minority carriers.
[0027]
【The invention's effect】
As is apparent from the above description, according to the present invention, the lifetime of minority carriers formed on the SOI layer on the surface of the support substrate can be measured in the middle of the semiconductor device manufacturing process by a very simple method. Thus, there is an advantage that a semiconductor substrate having a short minority carrier lifetime can be removed in the middle of the process, and a method for measuring the lifetime of minority carriers and a semiconductor device that can be expected to significantly improve the reliability and reliability. A manufacturing method can be provided.
[Brief description of the drawings]
FIG. 1 is a diagram showing the principle of the present invention. FIG. 2 is a diagram showing the relationship between the distance between an n + layer and an ion incident position and the amount of collected charges collected by a charge measuring instrument. Sectional view of an example [FIG. 4] Plan view of a first embodiment according to the present invention [FIG. 5] Sectional view of a second embodiment according to the present invention [FIG. 6] Plan view of a second embodiment according to the present invention [FIG. 7 is a sectional view of a third embodiment according to the present invention. FIG. 8 is a plan view of a third embodiment according to the present invention. FIG. 9 is a sectional view of a fourth embodiment according to the present invention.
1 Support substrate 2 Insulating film 3 SOI layer 4 p + layer
4a p + layer pad electrode 5 n + layer
5a n + layer pad electrode
6a Metal wiring
6b Metal wiring 7 ion
7a alpha source
7b α ray 8 Charge measuring instrument 9 Polyimide film
9a Polyimide hole
10 Gate electrode
10a Pad electrode of gate electrode
10b Gate oxide film
11 Silicon substrate
12 Oxide film
13 p-type silicon layer

Claims (5)

p型のSOI層にp+層とn+層を形成し、該p+層とn+層とをそれぞれp+層パッド電極とn+層パッド電極と接続するメタル配線層を備えた半導体装置における少数キャリアのライフタイムの測定法において、
前記n+層パッド電極とアースの間に電荷計測器を設け、前記p+層パッド電極をアースに接続し、前記p+層とn+層との間のSOI層にイオンを注入した際に前記電荷計測器により前記n+層パッド電極に収集された電荷量を計測し、前記イオンの注入位置と収集電荷量の関係に基づき、前記SOI層の少数キャリアのライフタイムを算出することを特徴とする少数キャリアのライフタイムの測定法。
A semiconductor device comprising a metal wiring layer in which ap + layer and an n + layer are formed in a p-type SOI layer, and the p + layer and the n + layer are connected to the p + layer pad electrode and the n + layer pad electrode, respectively. In the method of measuring the lifetime of minority carriers in
When a charge measuring device is provided between the n + layer pad electrode and the ground, the p + layer pad electrode is connected to the ground, and ions are implanted into the SOI layer between the p + layer and the n + layer The charge amount collected by the n + layer pad electrode is measured by the charge measuring device, and the lifetime of minority carriers in the SOI layer is calculated based on the relationship between the ion implantation position and the collected charge amount. Minority carrier lifetime measurement method.
前記メタル配線層の表面にα線を遮蔽する被膜を形成して該被膜に開口を設け、前記α線の放射線源を前記半導体装置の上に設け、前記開口の位置と収集電荷量の関係に基づき、前記SOI層の少数キャリアのライフタイムを算出することを特徴とする請求項1記載の少数キャリアのライフタイムの測定法。  Forming a coating that blocks α-rays on the surface of the metal wiring layer, providing an opening in the coating, providing the α-ray radiation source on the semiconductor device, and the relationship between the position of the opening and the amount of collected charge The minority carrier lifetime measurement method according to claim 1, wherein the minority carrier lifetime of the SOI layer is calculated based on the lifetime. 前記SOI層上にゲート電極を形成した後、前記SOI層にp+層とn+層を形成し、該ゲート電極に正の電圧を印加した状態において前記p+層とn+層との間のSOI層にイオンを注入した際に前記電荷計測器により前記n+層パッド電極に収集された電荷量を計測し、前記イオンの注入位置と収集電荷量の関係に基づき、前記SOI層の上側界面の少数キャリアのライフタイムを算出することを特徴とする請求項1記載の少数キャリアのライフタイムの測定法。After forming a gate electrode on the SOI layer, a p + layer and an n + layer are formed on the SOI layer, and a positive voltage is applied to the gate electrode between the p + layer and the n + layer. When the ions are implanted into the SOI layer, the charge amount collected by the n + layer pad electrode is measured by the charge meter, and the upper side of the SOI layer is measured based on the relationship between the ion implantation position and the collected charge amount. The minority carrier lifetime measurement method according to claim 1, wherein the lifetime of the minority carrier at the interface is calculated. 前記SOI層と支持基板間の酸化膜中に前記SOI層下面とゲート絶縁膜を介して接するゲート電極を形成した後、前記SOI層にp+層とn+層を形成し、該ゲート電極に正の電圧を印加した状態において前記p+層とn+層との間のSOI層にイオンを注入した際に前記電荷計測器により前記n+層パッド電極に収集された電荷量を計測し、前記イオンの注入位置と収集電荷量の関係に基づき、前記SOI層の下側界面の少数キャリアのライフタイムを算出することを特徴とする請求項1記載の少数キャリアのライフタイムの測定法。After forming a gate electrode in contact with the lower surface of the SOI layer via a gate insulating film in the oxide film between the SOI layer and the support substrate, a p + layer and an n + layer are formed on the SOI layer, and the gate electrode is formed on the gate electrode. Measuring the amount of charge collected on the n + layer pad electrode by the charge meter when ions are implanted into the SOI layer between the p + layer and the n + layer in a state where a positive voltage is applied; 2. The minority carrier lifetime measurement method according to claim 1, wherein the minority carrier lifetime of the lower interface of the SOI layer is calculated based on the relationship between the ion implantation position and the collected charge amount. 半導体装置の製造工程が、前記請求項1、2、3または4記載の方法により少数キャリアのライフタイムを測定する工程と、ライフタイムが設定値より短い半導体基板を除去する工程とを含むことを特徴とする半導体装置の製造方法。  The manufacturing process of a semiconductor device includes the step of measuring the lifetime of minority carriers by the method according to claim 1, 2, 3, or 4, and the step of removing a semiconductor substrate whose lifetime is shorter than a set value. A method of manufacturing a semiconductor device.
JP03015697A 1997-02-14 1997-02-14 Minority carrier lifetime measurement method and semiconductor device manufacturing method Expired - Fee Related JP3661334B2 (en)

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