IP Library › Granted Patent US 12,572,083
Granted Patent B2
US 12,572,083 · App. 18/255,543 · Granted Mar 10, 2026

Intensity order difference based metrology system, lithographic apparatus, and methods thereof

Inventors: Justin Lloyd Kreuzer (Trumbull, CT); Simon Reinald Huisman (Eindhoven, NL); Sebastianus Adrianus Goorden (Eindhoven, NL); Filippo Alpeggiani (Eindhoven, NL)
Assignees: ASML NETHERLANDS B.V.; ASML HOLDING N.V.
G03F7/70633G03F7/706837G03F7/706849
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Quick Facts
Patent No.
US 12,572,083
App. No.
18/255,543
Granted
Mar 10, 2026
Kind
B2
Abstract

The system includes a radiation source, a diffractive element, an optical system, a detector, and a processor. The radiation source generates radiation. The diffractive element diffracts the radiation to generate a first beam and a second beam. The first beam includes a first non-zero diffraction order and the second beam includes a second non-zero diffraction order that is different from the first non-zero diffraction order. The optical system receives a first scattered beam and a second scattered radiation beam from a target structure and directs the first scattered beam and the second scattered beam towards a detector. The detector generates a detection signal. The processor analyzes the detection signal to determine a target structure property based on at least the detection signal. The first beam is attenuated with respect to the second beam or the first scattered beam is purposely attenuated with respect to the second scattered beam.

Claims (37)

1 . A system comprising:

a radiation source configured to generate incoherent radiation;

a diffractive element configured to diffract the incoherent radiation to generate a first beam and a second beam, wherein the first beam comprises a first non-zero diffraction order and the second beam comprises a second non-zero diffraction order that is different from the first non-zero diffraction order;

an optical system configured to:

direct the first beam and the second beam towards a target structure,

receive a first scattered beam and a second scattered beam of radiation from the target structure,

direct the first scattered beam and the second scattered beam towards a detector, and

apodize one of the first beam or the second beam using an optical filter;

the detector configured to generate a detection signal;

a processor configured to:

analyze the detection signal to determine a fringe intensity between the first scattered beam and the second scattered beam based on an AC component and a DC component of the detection signal to determine an intensity imbalance, and

use the intensity imbalance to determine asymmetry of the target structure,

wherein the optical system comprises an optical element configured to attenuate the first beam with respect to the second beam or the first scattered beam with respect to the second scattered beam.

2 . The system of claim 1 , wherein the optical element is positioned between the radiation source and the optical system and configured to attenuate the first beam with respect to the second beam.

3 . The system of claim 1 , wherein the optical element positioned in an optical path of the first scattered beam between the target structure and the detector and configured to attenuate the first scattered beam with respect to the second scattered beam.

4 . The system of claim 1 , wherein the property of the target structure comprises a metrology mark symmetry.

5 . The system of claim 1 , wherein the first beam is associated with a positive diffraction order and the second beam is associated with a negative diffraction order.

6 . The system of claim 1 , wherein the target structure has an enhanced optical response that creates the intensity imbalance between the first scattered beam and the second scattered beam.

7 . A method comprising:

diffracting an incoherent radiation beam to generate a first beam and a second beam, wherein the first beam comprises a first non-zero diffraction order and the second beam comprises a second non-zero diffraction order that is different from the first non-zero diffraction order;

apodizing or attenuating one of the first beam or the second beam using an optical filter;

irradiating a target structure with the first beam and the second beam;

receiving a first scattered beam and a second scattered beam of radiation from the target structure;

generating, by a detector, a detection signal based on the first scattered beam and the second scattered beam;

analyzing, by a processor, the detection signal to determine a fringe intensity between the first scattered beam and the second scattered beam based on an AC component and a DC component of the detection signal to determine an intensity imbalance; and

using the intensity imbalance to determine asymmetry of the target structure.

8 . The method of claim 7 , further comprising passing one of the first scattered beam or the second scattered beam through an amplitude and/or phase apodizing filter.

9 . A method comprising:

irradiating a target structure with first and second incoherent radiation beams;

apodizing or attenuating one of the first beam or the second beam;

receiving a first scattered beam and a second scattered beam of radiation from the target structure;

generating a detection signal using an imaging detector based on the first scattered beam and the second scattered beam;

analyzing the detection signal to determine a fringe intensity between the first scattered beam and the second scattered beam based on an AC component and a DC component of the detection signal to determine an intensity imbalance; and

using the intensity imbalance to determine asymmetry of the target structure.

10 . The method of claim 9 , wherein the target structure has an enhanced optical response that creates the intensity imbalance between the first scattered beam and the second scattered beam and wherein the enhanced optical response is achieved by providing a sub-segmented metrology mark, the target structure comprising the sub-segmented metrology mark.

11 . The method of claim 9 , further comprising:

identifying a model between the intensity imbalance and the AC component and a DC component of the detection signal based on at least an illumination profile of the radiation beam.

Assignments (2)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jul 22, 2024
From: KREUZER, JUSTIN LLOYD
To: ASML HOLDING N.V.
Reel/Frame 068041/0168 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jul 22, 2024
From: HUISMAN, SIMON REINALD; GOORDEN, SEBASTIANUS ADRIANUS; ALPEGGIANI, FILIPPO
To: ASML NETHERLANDS B.V.
Reel/Frame 068041/0312 →
Continuity (3)
Provisional Application 63216355 · Jun 29, 2021
Provisional Application 63123548 · Dec 10, 2020
Related Publication 20240094641A1 · Mar 21, 2024
References Cited (42)
US 6297876B1 · Bornebroek · 2001 [cited by applicant]
US 6961116B2 · Den Boef et al. · 2005 [cited by applicant]
US 7511799B2 · Tel et al. · 2009 [cited by applicant]
US 8706442B2 · Mos et al. · 2014 [cited by applicant]
US 9784987B2 · Hill et al. · 2017 [cited by applicant]
US 9946167B2 · Smilde et al. · 2018 [cited by applicant]
US 10133188B2 · Jak et al. · 2018 [cited by applicant]
US 10152654B2 · Pandev · 2018 [cited by applicant]
US 10732516B2 · Pandev et al. · 2020 [cited by applicant]
US 11360399B2 · Goorden et al. · 2022 [cited by applicant]
US 11971665B2 · Adams · 2024 [cited by examiner]
US 12025925B2 · Alpeggiani · 2024 [cited by examiner]
US 20050094153A1 · Nikoonahad et al. · 2005 [cited by applicant]
US 20120123581A1 · Smilde et al. · 2012 [cited by applicant]
US 20140146322A1 · Hill et al. · 2014 [cited by applicant]
US 20150204664A1 · Bringoltz · 2015 [cited by examiner]
US 20160011523A1 · Singh · 2016 [cited by examiner]
US 20180224753A1 · Mathijssen et al. · 2018 [cited by applicant]
US 20190204759A1 · Shome · 2019 [cited by examiner]
US 20200209608A1 · Beukman et al. · 2020 [cited by applicant]
US 20210132509A1 · Huisman · 2021 [cited by examiner]
US 20220197151A1 · Mehta · 2022 [cited by examiner]
US 20230213871A1 · Goorden · 2023 [cited by examiner]
US 20230273531A1 · Swillam · 2023 [cited by examiner]
US 20230324817A1 · Ebert · 2023 [cited by examiner]
US 20230400782A1 · Cappelli · 2023 [cited by examiner]
US 20240036485A1 · Beukman · 2024 [cited by examiner]
US 20240077308A1 · Swillam · 2024 [cited by examiner]
US 20240160110A1 · Winters · 2024 [cited by examiner]
US 20240263941A1 · Cheng · 2024 [cited by examiner]
US 20250028258A1 · Voznyi · 2025 [cited by examiner]
TW 201229496A · 2012 [cited by applicant]
TW 201428262A · 2014 [cited by applicant]
TW 202014672A · 2020 [cited by applicant]
TW 202018430A · 2020 [cited by applicant]
TW 202028874A · 2020 [cited by applicant]
WO WO2020057900A1 · 2020 [cited by applicant]
International Search Report and Written Opinion of the International Searching Authority directed to International Patent Application No. PCT/EP2021/084056, mailed Apr. 8, 2022; 16 pages. [cited by applicant]
International Preliminary Report on Patentability directed to International Patent Application No. PCT/EP2021/084056, issued Jun. 13, 2023; 13 pages. [cited by applicant]
Niu et al., “Specular Spectroscopic Scatterometry in DUV Lithography,” Proc. SPIE, vol. 3677, Metrology, Inspection, and Process Control for Microlithography XIII, Jun. 14, 1999; 10 pages. [cited by applicant]
Raymond et al., “Multiparameter grating metrology using optical scatterometry,” Proc. SPIE, vol. 2725, Metrology, Inspection, and Process Control for Microlithography X, May 21, 1996; pp. 361-368. [cited by applicant]
“Lithographic Apparatus, Metrology Systems, and Methods Thereof,” Research Disclosure No. 676036, Jul. 7, 2020; 51 pages. [cited by applicant]