JPH0574937B2 - - Google Patents
Info
- Publication number
- JPH0574937B2 JPH0574937B2 JP59234930A JP23493084A JPH0574937B2 JP H0574937 B2 JPH0574937 B2 JP H0574937B2 JP 59234930 A JP59234930 A JP 59234930A JP 23493084 A JP23493084 A JP 23493084A JP H0574937 B2 JPH0574937 B2 JP H0574937B2
- Authority
- JP
- Japan
- Prior art keywords
- wafer
- microwave
- temperature
- sample
- semiconductor
- 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 - Lifetime
Links
Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10P—GENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
- H10P74/00—Testing 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】
〔発明の利用分野〕
本発明は半導体ウエハの電気特性評価装置に係
り、特に半導体内のキヤリア捕獲準位の非破壊測
定に好適な構成に係る。DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to an apparatus for evaluating electrical characteristics of semiconductor wafers, and particularly to a configuration suitable for non-destructive measurement of carrier trap levels within a semiconductor.
半導体のキヤリア寿命を測定する方法として、
光又は電子線励起による自由キヤリアの数が過渡
減衰する現象を自由キヤリア数の変化に伴なうマ
イクロ波吸収率の変化で測定する方法がある。
(参考文献1;宇佐美晶「非接触方式によるシリ
コンウエハライフタイム測定技術」、電子材料
(1981年2年号)p.67、参考文献2:特開昭59−
55013号公報)この測定をウエハ半導体結晶を試
料として行なうマイクロ波吸収率はウエハからの
反射マイクロ波を検出する方式がウエハ形状に制
限がなく実用的である。この方式を用いた例とし
ては参考文献2の「発明の実施例)に述べられて
いるが、この公知例を代表とする従来の測定装置
はキヤリア寿命の室温における値のみを測定する
事を目的としており、本発明の目的であるキヤリ
ア捕獲準位の精密測定については考慮されていな
い。従つて本発明の特徴である
1 試料ウエハの温度を制御する機構
2 低温域での試料表面への水蒸気の付着を防ぐ
機構
等を備えた例は無い。
As a method to measure the carrier life of semiconductors,
There is a method of measuring the phenomenon of transient attenuation of the number of free carriers due to light or electron beam excitation by measuring the change in microwave absorption rate accompanying the change in the number of free carriers.
(Reference 1: Akira Usami, “Silicon wafer lifetime measurement technology using non-contact method”, Electronic Materials (1981, 2nd issue) p. 67, Reference 2: Japanese Patent Application Laid-Open No. 1983-1999-
(No. 55013) This measurement of the microwave absorption rate using a wafer semiconductor crystal as a sample involves detecting reflected microwaves from the wafer, which is practical as there is no restriction on the wafer shape. An example of using this method is described in "Embodiments of the Invention" in Reference 2, but conventional measuring devices such as this known example are intended to measure only the value of carrier life at room temperature. Therefore, the precise measurement of the carrier capture level, which is the purpose of the present invention, is not considered.Therefore, the characteristics of the present invention are 1. Mechanism for controlling the temperature of the sample wafer 2. Water vapor on the sample surface in a low temperature range There are no examples that have a mechanism to prevent the adhesion of.
本発明の目的は、半導体ウエハ内のキヤリア捕
獲準位を非破壊で測定する為の結晶評価装置を提
供することにある。
An object of the present invention is to provide a crystal evaluation device for non-destructively measuring carrier trap levels within a semiconductor wafer.
本発明の特徴は、光ビーム又は電子ビームとマ
イクロ波とをウエハ状半導体結晶表面の同一領域
(光又は電子ビームの照射領域がマイクロ波照射
領域内に完全に含まれていてもよい。また逆にマ
イクロ波照射領域が光または電子ビーム照射領域
に完全に含まれていてもよい。)に照射する機能
を持つ装置に、(1)試料ウエハ温度を液体窒素温度
から室温以上の温度領域で温度を一定に保つ機構
と、(2)試料ウエハを真空状態に保ち、ウエハ表面
への水蒸気の付着を防ぐ機能とを付加した点にあ
る。先ず(2)の機能によつて低温域での反射マイク
ロ波強度の測定が高精度で行なう事が可能になつ
た。また(1)の機能は従来考慮されていなかつた新
しい機能で、この機能よりキヤリア捕獲準位の高
精度測定が可能となつた。
A feature of the present invention is that the light beam or electron beam and the microwave are applied to the same area on the surface of a wafer-like semiconductor crystal (the irradiation area of the light or electron beam may be completely included within the microwave irradiation area, or vice versa). (The microwave irradiation area may be completely included in the light or electron beam irradiation area.) and (2) a function to keep the sample wafer in a vacuum state and prevent water vapor from adhering to the wafer surface. First, the function (2) makes it possible to measure the reflected microwave intensity at low temperatures with high accuracy. In addition, function (1) is a new function that has not been considered in the past, and this function makes it possible to measure the carrier capture level with high accuracy.
以下本発明の実施例を図面を用いて説明する。
まず、第1図に示すように、液体窒素を溜め試料
を冷却する能力を持つ試料台8が、マイクロ波導
波管4と先端の窓材5を設けた蓋1と、本体3、
Oリング2、真空ポンプ13からなる真空容器内
に設置されており、試料ウエハを真空状態に保
つ。このため、導波管4と蓋1及び導波管の先端
と窓材5との間はそれぞれ真空気密を保つよう設
計されている。
Embodiments of the present invention will be described below with reference to the drawings.
First, as shown in FIG. 1, a sample stage 8, which has the ability to store liquid nitrogen and cool the sample, consists of a lid 1 provided with a microwave waveguide 4 and a window material 5 at the tip, a main body 3,
It is installed in a vacuum container consisting of an O-ring 2 and a vacuum pump 13, and keeps the sample wafer in a vacuum state. For this reason, the spaces between the waveguide 4 and the lid 1, and between the tip of the waveguide and the window material 5 are designed to maintain vacuum tightness.
また試料台8には液体窒素タンク6、液体窒素
供給管11、気化した窒素の排気管12及び冷却
用フイン7から成る冷却システムと、ヒータ9が
設けられ、ヒータへの電流値と液体窒素供給量を
調節する事により試料14の温度を液体窒素温度
から室温以上の温度範囲で一定に保つ事ができ
る。 The sample stage 8 is also provided with a cooling system consisting of a liquid nitrogen tank 6, a liquid nitrogen supply pipe 11, a vaporized nitrogen exhaust pipe 12, and a cooling fin 7, and a heater 9, which controls the current value and liquid nitrogen supply to the heater. By adjusting the amount, the temperature of the sample 14 can be kept constant in the temperature range from liquid nitrogen temperature to room temperature or higher.
試料14が温度調節機構により所定の温度に安
定した後、光または電子ビーム15窓材5を通し
て照射し試料ウエハ内に自由キヤリアを発生させ
る。またビーム15の照射領域を含む形でマイク
ロ波を導波管4を経て照射し、そのウエハからの
反射波は再び4を経て検出器で電気信号に変換さ
れる。 After the sample 14 is stabilized at a predetermined temperature by the temperature control mechanism, a light or electron beam 15 is irradiated through the window material 5 to generate free carriers within the sample wafer. Furthermore, microwaves are irradiated through the waveguide 4 in a manner that includes the irradiation area of the beam 15, and the reflected wave from the wafer passes through the wafer 4 again and is converted into an electrical signal by a detector.
第2図はキアリア寿命測定のための全測定系を
表わしている。23は第1図を用いて説明した真
空容器を模式的に表わしており、同様に24は第
1図で示した試料台部分を模式的に表わしてい
る。以下第2図を用いて測定系の構成を説明す
る。先ずマイクロ波発生器16で発生したマイク
ロ波19はサーキユレータ17を経て20の経路
でウエハ状試料25に定常的に照射される。また
試料上のマイクロ波照射領域の中にパルス化され
た電子又は光ビームが照射され、ウエハ試料内に
自由キヤリアを周期的に励起する。この結果、ウ
エハ試料表面からの反射マイクロ波20,21は
サーキユレータ17を経てマイクロ波検出器18
で電気信号に変換されるが、この信号はキヤリア
励起に用いたビームの変調周期で変調を受ける。
従つて信号増幅器27からの信号をビーム発生器
28からの周期信号で同期させ、オシロスコープ
30で観察すると、ビーム遮断直後の波形は指数
関数的な減衰波形となり、その時定数からキイリ
ア寿命τが求まる。オシロコープ30の信号と、
温度検出器26,29からの信号はコンピユータ
31に伝導されキヤリア寿命τの温度依存性が求
められる。 FIG. 2 represents the entire measurement system for measuring Chiaria lifespan. Reference numeral 23 schematically represents the vacuum vessel described using FIG. 1, and similarly, 24 schematically represents the sample stage portion shown in FIG. The configuration of the measurement system will be explained below using FIG. 2. First, the microwave 19 generated by the microwave generator 16 passes through the circulator 17 and is constantly irradiated onto the wafer-shaped sample 25 through 20 routes. A pulsed electron or light beam is also directed into the microwave irradiation region on the sample to periodically excite free carriers within the wafer sample. As a result, the reflected microwaves 20 and 21 from the wafer sample surface pass through the circulator 17 to the microwave detector 18.
This signal is converted into an electrical signal, but this signal is modulated by the modulation period of the beam used for carrier excitation.
Therefore, when the signal from the signal amplifier 27 is synchronized with the periodic signal from the beam generator 28 and observed with an oscilloscope 30, the waveform immediately after the beam is cut off becomes an exponential decay waveform, and the key carrier life τ can be determined from its time constant. Oscilloscope 30 signal and
Signals from the temperature detectors 26 and 29 are transmitted to a computer 31 to determine the temperature dependence of the carrier life τ.
本実施例によれば、第1図のマイクロ波導波管
4とウエハ状試料14の相対位置を1mm程度にま
でに近づける事が可能である。従つてマイクロ波
がウエハ試料表面が拡がつてしまう事なく照射さ
れるので反射マイクロ波の強度も大きくなり信号
の検出感度を大きくする効果がある。また真空容
器と導波管を一体化させた事により、ウエハ状試
料と導波管端面との相対位置を常に一定に保つ事
ができるので、再現性の高い測定が可能である。
また信号をマイクロ波で検出する方式であるた
め、従来電極を試料上に作製し電気信号を検出す
る方式では困難であつた高抵抗体(例えば10S
Ω・cm程度の比抵抗を持つ半絶縁性GaAs)内の
キヤリア寿命、キヤリア捕獲準位の測定が容易に
行なえるという効果がある。 According to this embodiment, it is possible to bring the relative positions of the microwave waveguide 4 and the wafer-shaped sample 14 in FIG. 1 close to about 1 mm. Therefore, since the microwave is irradiated without spreading the surface of the wafer sample, the intensity of the reflected microwave increases, which has the effect of increasing signal detection sensitivity. Furthermore, by integrating the vacuum container and the waveguide, the relative position between the wafer-shaped sample and the end face of the waveguide can always be kept constant, making it possible to perform highly reproducible measurements.
In addition, since the signal is detected using microwaves, it is difficult to detect electric signals using high-resistance materials (for example, 10 S
This method has the effect of making it easy to measure the carrier lifetime and carrier trapping level in semi-insulating GaAs (semi-insulating GaAs, which has a resistivity of about Ωcm).
本発明によれば従来困難であつたウエハ状結晶
のキヤリア捕獲準位の高精度非破壊測定が可能と
なるという効果がある。
According to the present invention, it is possible to perform highly accurate non-destructive measurement of the carrier trapping level of a wafer-shaped crystal, which has been difficult in the past.
第1図は試料台部分の断面図であり、第2図は
キヤリア寿命測定系の構成を示す装置構成図であ
る。
1……真空容器の蓋、2……Oリング、3……
真空容器本体、4……マイクロ波導波管、5……
真空封止用窓材、6……液体窒素タンク、7……
冷却用フイン、8……試料台、9……ヒータ、1
0……液体窒素、11……液体窒素供給用パイ
プ、12……窒素ガス排気管、13……真空ポン
プ、14……試料ウエハ、15……電子ビーム又
は光ビーム、16……マイクロ波発生器、17…
…サーキユレータ、18……マイクロ波検出器、
19……入射マイクロ波、20……入射及び反射
マイクロ波、21……反射マイクロ波、22……
電子ビーム又は光ビーム、23……真空容器、2
4……試料台、25……試料ウエハ、26……温
度検出器、27……信号増幅器、28……ビーム
発生器、29……温度測定器、30……オシロス
コープ、31……系制御及び信号処理用コンピユ
ータ。
FIG. 1 is a cross-sectional view of a sample stage portion, and FIG. 2 is an apparatus configuration diagram showing the configuration of a carrier life measurement system. 1...Lid of vacuum container, 2...O ring, 3...
Vacuum container body, 4...Microwave waveguide, 5...
Vacuum sealing window material, 6...Liquid nitrogen tank, 7...
Cooling fin, 8...Sample stand, 9...Heater, 1
0... Liquid nitrogen, 11... Liquid nitrogen supply pipe, 12... Nitrogen gas exhaust pipe, 13... Vacuum pump, 14... Sample wafer, 15... Electron beam or light beam, 16... Microwave generation Vessel, 17...
...Circulator, 18...Microwave detector,
19...Incoming microwave, 20...Incoming and reflected microwave, 21...Reflected microwave, 22...
Electron beam or light beam, 23...vacuum container, 2
4... Sample stage, 25... Sample wafer, 26... Temperature detector, 27... Signal amplifier, 28... Beam generator, 29... Temperature measuring device, 30... Oscilloscope, 31... System control and Computer for signal processing.
Claims (1)
置する半導体ウエハの温度を制御するための手段
と、上記半導体ウエハ表面への水蒸気の付着を防
ぐ手段と、上記半導体ウエハにマイクロ波を照射
するための手段と、上記半導体ウエハ上のマイク
ロ波照射領域に光ビームまたは電子ビームを照射
するための手段と、上記半導体ウエハ表面からの
上記マイクロ波の反射波を検出するための手段を
有することを特徴とする半導体評価装置。 2 上記半導体ウエハ表面への水蒸気の付着を防
ぐ手段は真空容器であり、該真空容器には上記マ
イクロ波を照射するための手段と上記反射マイク
ロ波を検出するための手段を兼ねる導波管が設け
られており、該導波管の先端部には上記光ビーム
または電子ビームを照射するための手段である窓
材が設けられており、かつ上記真空容器内に上記
ウエハステージが設けられている特許請求の範囲
第1項記載の半導体評価装置。 3 上記温度を制御するため手段は液体窒素温度
から室温以上の温度範囲で温度を一定に保つ機能
を有する特許請求の範囲第1項又は第2項記載の
半導体評価装置。[Scope of Claims] 1. A wafer stage, a means for controlling the temperature of a semiconductor wafer placed on the wafer stage, a means for preventing water vapor from adhering to the surface of the semiconductor wafer, and a means for controlling the temperature of a semiconductor wafer placed on the wafer stage. means for irradiating a microwave irradiation area on the semiconductor wafer with a light beam or an electron beam; and means for detecting reflected waves of the microwave from the surface of the semiconductor wafer. A semiconductor evaluation device comprising: 2. The means for preventing water vapor from adhering to the surface of the semiconductor wafer is a vacuum container, and the vacuum container includes a waveguide that serves as a means for irradiating the microwave and a means for detecting the reflected microwave. A window material, which is a means for irradiating the light beam or electron beam, is provided at the tip of the waveguide, and the wafer stage is provided within the vacuum container. A semiconductor evaluation device according to claim 1. 3. The semiconductor evaluation device according to claim 1 or 2, wherein the means for controlling the temperature has a function of keeping the temperature constant in a temperature range from liquid nitrogen temperature to room temperature or higher.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59234930A JPS61114543A (en) | 1984-11-09 | 1984-11-09 | Semiconductor evaluating unit |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59234930A JPS61114543A (en) | 1984-11-09 | 1984-11-09 | Semiconductor evaluating unit |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61114543A JPS61114543A (en) | 1986-06-02 |
| JPH0574937B2 true JPH0574937B2 (en) | 1993-10-19 |
Family
ID=16978501
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59234930A Granted JPS61114543A (en) | 1984-11-09 | 1984-11-09 | Semiconductor evaluating unit |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61114543A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH06101506B2 (en) * | 1985-01-30 | 1994-12-12 | 三菱マテリアル株式会社 | Method for measuring EL2 distribution of gallium arsenide semiconductor wafer |
| JPH02248062A (en) * | 1989-03-20 | 1990-10-03 | Semitetsukusu:Kk | Lifetime measuring method and device of semiconductor element |
| JP5301770B2 (en) * | 2006-08-25 | 2013-09-25 | 株式会社神戸製鋼所 | Thin film semiconductor crystallinity measuring apparatus and method |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS53118373A (en) * | 1977-03-25 | 1978-10-16 | Mitsubishi Metal Corp | Method of measuring characteristic of semiconductor by microwave |
| JPS59114834A (en) * | 1982-12-21 | 1984-07-03 | Agency Of Ind Science & Technol | Method for measuring deep impurity level or crystal defect level contained in semiconductor device |
-
1984
- 1984-11-09 JP JP59234930A patent/JPS61114543A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61114543A (en) | 1986-06-02 |
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