The patent badge is an abbreviated version of the USPTO patent document. The patent badge does contain a link to the full patent document.

The patent badge is an abbreviated version of the USPTO patent document. The patent badge covers the following: Patent number, Date patent was issued, Date patent was filed, Title of the patent, Applicant, Inventor, Assignee, Attorney firm, Primary examiner, Assistant examiner, CPCs, and Abstract. The patent badge does contain a link to the full patent document (in Adobe Acrobat format, aka pdf). To download or print any patent click here.

Date of Patent:
Nov. 13, 2007

Filed:

Sep. 02, 2005
Applicants:

Nobuyuki Naka, Kyoto, JP;

Akihiro Katanishi, Kyoto, JP;

Masaaki Magari, Kyoto, JP;

Inventors:

Nobuyuki Naka, Kyoto, JP;

Akihiro Katanishi, Kyoto, JP;

Masaaki Magari, Kyoto, JP;

Assignee:

Horiba, Ltd., Kyoto, JP;

Attorney:
Primary Examiner:
Assistant Examiner:
Int. Cl.
CPC ...
G01J 3/44 (2006.01);
U.S. Cl.
CPC ...
Abstract

The present invention provides a method of and a device for measuring the stress in a semiconductor material. An excitation light is irradiated on a semiconductor material formed with a silicon germanium layer and a strained silicon layer in a multilayer structure on a single crystal silicon substrate from the direction of the strained silicon layer. An internal stress of the semiconductor material is measured from peak position information of the Raman spectrum of scattered light from the irradiating point, wherein light having a wavelength capable of reaching the single crystal silicon substrate is used as the excitation light, a temperature of the semiconductor material is estimated from a shift amount of the peak position of the Raman spectrum of the scattered light from the substrate in accordance with the irradiation of the excitation light and the shift amounts of the peak positions of the Raman spectra in the strained silicon layer and in the silicon germanium layer are corrected by means of the estimated temperature, The internal stresses of the strained silicon layer and the silicon germanium layer are calculated from the corrected peak position information of the Raman spectra in the respective layers.


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