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:
Sep. 08, 2020

Filed:

Nov. 21, 2018
Applicant:

National Technology & Engineering Solutions of Sandia, Llc, Albuquerque, NM (US);

Inventors:

David W. Chandler, Livermore, CA (US);

Kimberlee Chiyoko Celio, Berkeley, CA (US);

Attorney:
Primary Examiner:
Assistant Examiner:
Int. Cl.
CPC ...
H01J 37/244 (2006.01); H01J 37/12 (2006.01); H01J 37/06 (2006.01); H01J 37/28 (2006.01); H01J 37/22 (2006.01); H01J 37/20 (2006.01);
U.S. Cl.
CPC ...
H01J 37/244 (2013.01); H01J 37/06 (2013.01); H01J 37/12 (2013.01); H01J 37/20 (2013.01); H01J 37/22 (2013.01); H01J 37/28 (2013.01); H01J 2237/04735 (2013.01); H01J 2237/2443 (2013.01); H01J 2237/24585 (2013.01);
Abstract

A scanning electron microscope (SEM) system includes an SEM objective that emits an electron beam toward a sample, causing emission of charged particles including secondary electrons, Auger electrons, backscattered electrons, anions and cations. The SEM system includes electron optics elements that are configured to establish electric fields around the sample that accelerate charged particles toward a detector. A two-dimensional distribution of locations of incidence of the charged particles on the detector is indicative of energies of the charged particles and their emission angles from the sample. A three-dimensional spatial distribution of charged particles emitted from the sample is recovered by performing an Abel transform over the distribution on the detector. The energies and emission angles of the charged particles are then determined from the three-dimensional spatial distribution.


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