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:
Aug. 04, 2020

Filed:

Apr. 01, 2016
Applicant:

Intel Corporation, Santa Clara, CA (US);

Inventors:

Kevin P. O'Brien, Portland, OR (US);

Kaan Oguz, Beaverton, OR (US);

Christopher J. Wiegand, Portland, OR (US);

Mark L. Doczy, Beaverton, OR (US);

Brian S. Doyle, Portland, OR (US);

MD Tofizur Rahman, Portland, OR (US);

Oleg Golonzka, Beaverton, OR (US);

Tahir Ghani, Portland, OR (US);

Assignee:

Intel Corporation, Santa Clara, CA (US);

Attorney:
Primary Examiner:
Int. Cl.
CPC ...
G01R 31/28 (2006.01); H01L 43/12 (2006.01); G01R 33/09 (2006.01); G01R 31/315 (2006.01); H01L 21/66 (2006.01); G01R 33/60 (2006.01); G01N 24/10 (2006.01); G01R 35/00 (2006.01);
U.S. Cl.
CPC ...
G01R 31/2831 (2013.01); G01N 24/10 (2013.01); G01R 31/315 (2013.01); G01R 33/098 (2013.01); G01R 33/60 (2013.01); H01L 22/14 (2013.01); H01L 43/12 (2013.01); G01R 35/00 (2013.01);
Abstract

Techniques are disclosed for carrying out ferromagnetic resonance (FMR) testing on whole wafers populated with one or more buried magnetic layers. The techniques can be used to verify or troubleshoot processes for forming the buried magnetic layers, without requiring the wafer to be broken. The techniques can also be used to distinguish one magnetic layer from others in the same stack, based on a unique frequency response of that layer. One example methodology includes moving a wafer proximate to a waveguide (within 500 microns, but without shorting), energizing a DC magnetic field near the target measurement point, applying an RF input signal through the waveguide, collecting resonance spectra of the frequency response of the waveguide, and decomposing the resonance spectra into magnetic properties of the target layer. One or both of the DC magnetic field and RF input signal can be swept to generate a robust set of resonance spectra.


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