JPS6127904B2 - - Google Patents
Info
- Publication number
- JPS6127904B2 JPS6127904B2 JP52150579A JP15057977A JPS6127904B2 JP S6127904 B2 JPS6127904 B2 JP S6127904B2 JP 52150579 A JP52150579 A JP 52150579A JP 15057977 A JP15057977 A JP 15057977A JP S6127904 B2 JPS6127904 B2 JP S6127904B2
- Authority
- JP
- Japan
- Prior art keywords
- semiconductor
- measuring
- laser beam
- silicon wafer
- wavelength
- 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
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- Investigating Or Analysing Materials By Optical Means (AREA)
- Testing Or Measuring Of Semiconductors Or The Like (AREA)
Description
【発明の詳細な説明】
本発明は半導体の不純物濃度の測定方法、さら
に特定すれば、赤外波長領域の半導体レーザーを
用いて、シリコンウエハ中の酸素および炭素の濃
度の2次元分布を測定する方法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention provides a method for measuring the impurity concentration of a semiconductor, and more specifically, a method for measuring the two-dimensional distribution of oxygen and carbon concentrations in a silicon wafer using a semiconductor laser in the infrared wavelength region. Regarding the method.
シリコン結晶中に不純物として酸素および炭素
が存在するとき、赤外線ビームをこれに照射する
と、酸素で9.00μ、炭素で16.50μのビームが濃
度に応じて吸収される。この吸収係数を測定して
不純物濃度を評価することができる。 When oxygen and carbon exist as impurities in a silicon crystal, when irradiated with an infrared beam, oxygen absorbs a beam of 9.00μ and carbon absorbs a beam of 16.50μ depending on the concentration. The impurity concentration can be evaluated by measuring this absorption coefficient.
従来、赤外線の光源として炭化けい素などの抵
抗発熱体を利用し、これから放射する光を回折格
子またはプリズムによつて分光し、スリツトによ
つて特定波長領域のビームとする方法が行なわれ
た。この方法では、光源から放射する白光色を分
光するので、光強度が弱く、また抵抗発熱体の特
性によつて光ビーム径が大きい。従つて、シリコ
ンウエハ中の微小領域、すなわち1〜106μ2に
おける不純物濃度を測定することが原理的に不可
能であつた。 Conventionally, a method has been used in which a resistance heating element such as silicon carbide is used as an infrared light source, the light emitted from the element is separated into spectra using a diffraction grating or a prism, and a beam in a specific wavelength range is produced using a slit. In this method, the white light emitted from the light source is separated, so the light intensity is low, and the light beam diameter is large due to the characteristics of the resistive heating element. Therefore, it has been impossible in principle to measure the impurity concentration in a micro region, that is, 1 to 10 6 μ 2 in a silicon wafer.
光ビームの径を小さくする目的で、
Pb1―xSnxTe(x=0.10〜0.20)半導体レーザー
を光源とする方法が提唱されている。このレーザ
ービームは、ビーム径を1〜103μの範囲内に絞
ることができる。 In order to reduce the diameter of the light beam,
A method using a Pb 1 - x Sn x Te (x=0.10 to 0.20) semiconductor laser as a light source has been proposed. The beam diameter of this laser beam can be focused within the range of 1 to 10 3 μm.
本発明の方法は、上記半導体レーザーを光源と
し、これから放射するレーザー光を回折格子また
はプリズムによつて分光し、すなわち酸素原子の
分布を測定する場合は9.00μ、また炭素原子の場
合には16.50μのレーザービームに分光し、スリ
ツトによつてビーム径を20〜30μに絞る。このレ
ーザービームの光軸面に対して垂直な平面におい
て、シリコンウエハを駆動機構によつて自動的に
2次元的に移動させ、シリコンウエハに照射して
透過したレーザービームを測定する。これによつ
て、シリコンウエハの1〜106μ2程度の微小領
域ごとに存在する、酸素または炭素による吸収係
数を精度よくかつ迅速に測定し、これらの不純物
濃度を測定することができる。 The method of the present invention uses the above-mentioned semiconductor laser as a light source, and the laser light emitted from the laser beam is divided into spectra using a diffraction grating or a prism. In other words, when measuring the distribution of oxygen atoms, the distribution of oxygen atoms is 9.00μ, and when measuring the distribution of carbon atoms, it is 16.50μ. The laser beam is divided into μ laser beams, and the beam diameter is narrowed down to 20 to 30 μ using a slit. The silicon wafer is automatically moved two-dimensionally by a drive mechanism in a plane perpendicular to the optical axis plane of this laser beam, and the laser beam that is irradiated onto and transmitted through the silicon wafer is measured. Thereby, it is possible to accurately and quickly measure the absorption coefficient of oxygen or carbon present in each minute region of about 1 to 10 6 μ 2 on the silicon wafer, and to measure the concentration of these impurities.
第1図は本発明の方法において使用する分光系
の説明図である。Pb1―xSnxTe(x=0.10〜
0.20)半導体レーザー1をクライオスタツト2内
に収め、その温度を1〜100〓の範囲、好ましく
は77〓程度に保つ。電源3は0.1〜3Aの範囲の定
電流を安定して供給し、かつ定電流値を中心に±
500mAの電流掃引が可能である。酸素または炭
素の濃度を測定するときには、まずこの電流を
2A±500mAとして、発振するレーザービームの
波長を変化させて、不純物の吸収最大領域におけ
る波長を選ぶ。 FIG. 1 is an explanatory diagram of a spectroscopic system used in the method of the present invention. Pb 1 ― x Sn x Te (x=0.10~
0.20) The semiconductor laser 1 is housed in the cryostat 2, and its temperature is maintained in the range of 1 to 100〓, preferably around 77〓. Power supply 3 stably supplies constant current in the range of 0.1 to 3A, and ± around the constant current value.
500mA current sweep is possible. When measuring the concentration of oxygen or carbon, first this current is
At 2A±500mA, change the wavelength of the oscillated laser beam and select the wavelength in the maximum absorption region of impurities.
こうして、レーザー1から放射するレーザービ
ームはレンズ4を通して収束した後に、回折格子
分光系5によつて分光し、検知すべき不純物が酸
素のときは9.00μ、また炭素のときは16.50μと
して取り出し、その後にレンズ6でレーザービー
ムを収束させ、さらにスリツト7によつてビーム
径を30μに絞る。シリコンウエハ試料8は試料駆
動装置9によつて、光軸に対して垂直な平面内
で、レーザービームの径と同じ30μ間隔で2次元
的に移動させる。試料8を透過した光はHgCdTe
半導体検知器10によつて光強度を測定し、検知
器10の出力を増幅器11で増幅して記録計12
で記録する。 In this way, the laser beam emitted from the laser 1 is converged through the lens 4, and then separated into spectra by the diffraction grating spectrometer 5. When the impurity to be detected is oxygen, it is extracted as 9.00μ, and when it is carbon, it is extracted as 16.50μ. Thereafter, the laser beam is converged with a lens 6, and further narrowed down to a beam diameter of 30 μm with a slit 7. The silicon wafer sample 8 is two-dimensionally moved by a sample drive device 9 in a plane perpendicular to the optical axis at intervals of 30 μm, which is the same as the diameter of the laser beam. The light transmitted through sample 8 is HgCdTe
The light intensity is measured by a semiconductor detector 10, the output of the detector 10 is amplified by an amplifier 11, and the output is amplified by a recorder 12.
Record with .
以上述べた様に本発明によればレーザービーム
により半導体を走査する様にしているので、2次
元的な不純物濃度の測定が可能である。又レーザ
ービームであるので局部的な不純物濃度の測定も
可能となる。 As described above, according to the present invention, since the semiconductor is scanned with a laser beam, it is possible to measure the impurity concentration two-dimensionally. Furthermore, since it is a laser beam, it is also possible to measure local impurity concentrations.
第1図は本発明の方法を実施する装置の説明図
である。
1……化合物半導体レーザー、2……クライオ
スタツト、3……定電流電源、4,6……レン
ズ、5……回折格子分光系、7……スリツト、8
……シリコンウエハ試料、9……試料駆動装置、
10……検知器、11……増幅器、12……記録
計。
FIG. 1 is an explanatory diagram of an apparatus for carrying out the method of the present invention. 1... Compound semiconductor laser, 2... Cryostat, 3... Constant current power supply, 4, 6... Lens, 5... Diffraction grating spectroscopy system, 7... Slit, 8
...Silicon wafer sample, 9...Sample driving device,
10...detector, 11...amplifier, 12...recorder.
Claims (1)
することにより、この半導体の不純物濃度を測定
する方法において、波長可変型あるPb1―xSnxTe
(x=0.10〜0.20)半導体レーザーの温度および
発振電流を制御して、レーザービームの波長を前
記不純物の最大吸収波長に固定して、前記半導体
であるシリコンウエハに照射し、透過したレーザ
ービームをHgCdTe半導体検知器により光強度を
測定するとともに、このシリコンウエハと前記レ
ーザービームとを相対的に移動させることによつ
て、シリコンウエハ中の前記不純物の2次元分布
を測定することを特徴とする、半導体の不純物濃
度の測定方法。1 In a method of measuring the impurity concentration of a semiconductor by irradiating the semiconductor with a light beam and measuring the absorption coefficient, a wavelength-tunable Pb 1 - x Sn x Te
(x = 0.10 to 0.20) By controlling the temperature and oscillation current of the semiconductor laser, the wavelength of the laser beam is fixed to the maximum absorption wavelength of the impurity, and the silicon wafer, which is the semiconductor, is irradiated, and the transmitted laser beam is The two-dimensional distribution of the impurities in the silicon wafer is measured by measuring the light intensity with an HgCdTe semiconductor detector and by moving the silicon wafer and the laser beam relatively. Method for measuring impurity concentration in semiconductors.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15057977A JPS5483371A (en) | 1977-12-16 | 1977-12-16 | Measurement method of impurity concentration of semiconductor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15057977A JPS5483371A (en) | 1977-12-16 | 1977-12-16 | Measurement method of impurity concentration of semiconductor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5483371A JPS5483371A (en) | 1979-07-03 |
| JPS6127904B2 true JPS6127904B2 (en) | 1986-06-27 |
Family
ID=15499959
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP15057977A Granted JPS5483371A (en) | 1977-12-16 | 1977-12-16 | Measurement method of impurity concentration of semiconductor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5483371A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS56103351A (en) * | 1980-01-22 | 1981-08-18 | Fujitsu Ltd | Method for measuring impurity concentration of semiconductor |
| JPS59116038A (en) * | 1982-12-22 | 1984-07-04 | Taizo Ishikawa | Method for flaw detection using monochromatic light source |
| GB2550897B (en) * | 2016-05-27 | 2020-12-23 | Oxford Instruments Nanotechnology Tools Ltd | Cryogenic cooling system |
| WO2025234406A1 (en) * | 2024-05-10 | 2025-11-13 | 国立大学法人東北大学 | Nanoparticle distribution measurement method, distribution measurement device, and multilayer body manufacturing method and manufacturing device |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3767304A (en) * | 1972-07-03 | 1973-10-23 | Ibm | Apparatus and method for detection of internal semiconductor inclusions |
-
1977
- 1977-12-16 JP JP15057977A patent/JPS5483371A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5483371A (en) | 1979-07-03 |
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