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. 05, 2017

Filed:

Jul. 08, 2015
Applicant:

Asml Netherlands B.v., Veldhoven, NL;

Inventors:

Amandev Singh, Eindhoven, NL;

Henricus Petrus Maria Pellemans, Veldhoven, NL;

Patrick Warnaar, Tilburg, NL;

Assignee:

ASML Netherlands B.V., Veldhoven, NL;

Attorney:
Primary Examiner:
Int. Cl.
CPC ...
G03B 27/52 (2006.01); G03B 27/32 (2006.01); G03F 7/20 (2006.01); G01J 3/28 (2006.01); G01J 3/45 (2006.01); G01N 21/47 (2006.01);
U.S. Cl.
CPC ...
G03F 7/70491 (2013.01); G01J 3/2823 (2013.01); G01J 3/45 (2013.01); G01N 21/4788 (2013.01); G03F 7/70625 (2013.01); G03F 7/70633 (2013.01); G01N 2201/06113 (2013.01);
Abstract

Inspection apparatus () is used for measuring parameters of targets on a substrate. Coherent radiation follows an illumination path (solid rays) for illuminating target (T). A collection path (dashed rays) collects diffracted radiation from the target and delivers it to a lock-in image detector (). A reference beam following a reference path (dotted rays). An acousto-optical modulator () shifts the optical frequency of the reference beam so that the intensity of radiation at the lock-in detector includes a time-varying component having a characteristic frequency corresponding to a difference between the frequencies of the diffracted radiation and the reference radiation. The lock-in image detector records two-dimensional image information representing both amplitude and phase of the time-varying component. A second reference beam with a different shift () follows a second reference path (dot-dash rays). Interference between the two reference beams can be used for intensity normalization.


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