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. 05, 2019

Filed:

Mar. 02, 2016
Applicant:

Fraunhofer-gesellschaft Zur Foerderung Der Angewandten Forschung E.v., Munich, DE;

Inventors:

Philipp Wollmann, Dresden, DE;

Wulf Graehlert, Dresden, DE;

Eric Weissenborn, Dresden, DE;

Attorney:
Primary Examiner:
Assistant Examiner:
Int. Cl.
CPC ...
G01R 1/07 (2006.01); G01R 27/26 (2006.01); G01N 21/84 (2006.01); G01N 27/04 (2006.01);
U.S. Cl.
CPC ...
G01R 1/071 (2013.01); G01N 21/8422 (2013.01); G01N 27/04 (2013.01); G01R 27/2682 (2013.01); G01N 2021/8438 (2013.01);
Abstract

An arrangement for a spatially resolved determination of the specific electrical resistance and/or of the specific electrical conductivity of a sample at different positions, in which a plurality of detectors are configured for a spatially resolved spectral analysis of electromagnetic radiation within a wavelength interval and is incident onto the detectors. A radiation onto a surface takes place with homogeneous intensity. The measurement signals of the detectors detected with spatial resolution and wavelength resolution within a wavelength interval are compared for each detected position with a wavelength-resolved function that are compared by calculation of the propagation of electromagnetic radiation in multilayer systems while using an optical model for a physical description of the examined sample while taking account of the wavelength-dependent progressions of the linear optical refractive indices n and of the coefficients of absorption k of all the materials and/or substances forming the sample that can be approximated by a physical function of a complex refractive index of the conductive material or substance. They are brought to a sufficient overlap with a calibration curve progression by a change of the parameters of the physical function to determine the specific electrical resistance and/or the specific electrical conductivity at different positions with spatial resolution.


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