Prosecution Insights
Last updated: April 19, 2026
Application No. 18/513,481

CHARGED PARTICLE OPTICAL DEVICE, OBJECTIVE LENS ASSEMBLY, DETECTOR, DETECTOR ARRAY, AND METHODS

Non-Final OA §102§103
Filed
Nov 17, 2023
Examiner
CHANG, HANWAY
Art Unit
2878
Tech Center
2800 — Semiconductors & Electrical Systems
Assignee
ASML Netherlands B.V.
OA Round
1 (Non-Final)
86%
Grant Probability
Favorable
1-2
OA Rounds
2y 3m
To Grant
94%
With Interview

Examiner Intelligence

Grants 86% — above average
86%
Career Allow Rate
538 granted / 626 resolved
+17.9% vs TC avg
Moderate +8% lift
Without
With
+7.6%
Interview Lift
resolved cases with interview
Typical timeline
2y 3m
Avg Prosecution
65 currently pending
Career history
691
Total Applications
across all art units

Statute-Specific Performance

§101
1.5%
-38.5% vs TC avg
§103
38.4%
-1.6% vs TC avg
§102
34.8%
-5.2% vs TC avg
§112
6.0%
-34.0% vs TC avg
Black line = Tech Center average estimate • Based on career data from 626 resolved cases

Office Action

§102 §103
DETAILED ACTION Claim Rejections - 35 USC § 102 The following is a quotation of the appropriate paragraphs of 35 U.S.C. 102 that form the basis for the rejections under this section made in this Office action: A person shall be entitled to a patent unless – (a)(1) the claimed invention was patented, described in a printed publication, or in public use, on sale, or otherwise available to the public before the effective filing date of the claimed invention. Claims 1 and 3-15 are rejected under 35 U.S.C. 102(a)(1) as being anticipated by Wieland (US PGPub 2021/0210309, hereinafter Wieland). Regarding claim 1, Wieland discloses a charged particle optical device for a charged particle beam (charged particle assessment tool, see abstract), the device being configured to project an array of beams of charged particles along primary beam paths towards a sample (three sub-beams 311-313 are projected toward a sample 208, see paragraph [0070]), the device comprising: an objective lens array configured to project the beams onto a sample and comprising at least two electrodes along primary beam paths of an array of beams of charged particles (objective lens 331 projects three sub-beams 311-313 toward a sample 308, see Fig. 3 and paragraph [0070]; objective lens 401 depicted in more detail including electrodes in Fig. 4); an up-beam array of detectors positioned up-beam of at least one electrode along the primary beam paths of the at least two electrodes (sensor unit 503 is mounted to the upper electrode of objective lens 501, see paragraph [0121]) a down-beam array of detectors positioned down-beam of the at least one electrode along the primary beam path (array of detector modules 402, see Fig. 4-5 and paragraph [0091]; located downstream of electrodes of objective lens 401, see Fig. 4; both embodiments of the sensor units 503 of the upper electrode and detection device 240 of the lower electrodes may be integrated with objective lens 501, see paragraph [0121]); at least one voltage supply configured to be electrically connected to the objective lens array (voltage supply (not shown) applies potentials to the electrodes of the objective lens, see paragraph [0125]); and a controller configured to control a potential applied by the at least one voltage supply to the at least one electrode of the objective lens array (voltage supply (not shown) applies potentials to the electrodes of the objective lens, see paragraph [0125]; controller configured to control potentials applied to the electrodes of the control lenses and the objective lenses to affect the landing energy for detection, see paragraph [0135]); wherein the up-beam array of detectors and the down-beam array of detectors are configured simultaneously to detect signal particles (both embodiments of the sensor units 503 of the upper electrode and detection device 240 of the lower electrodes may be integrated with objective lens 501, see paragraph [0121], for detection). Regarding claim 3, Wieland discloses the down-beam array of detectors is positioned down-beam of the objective lens array along the primary beam paths and facing the sample in use (on the output side of the objective lens 401, the side facing the sample 208, a detector module 402 is provided, see paragraph [0091]). Regarding claim 4, Wieland discloses a potential of the down-beam array of detectors relative to a potential of the sample is selected to control detection of the signal particles by the down-beam array of detectors, preferably the control in detection of the signal particles is in an energy range of the signal particles with respect to the respective primary beam paths (controller configured to control potentials applied to the electrodes of the control lenses and the objective lenses to affect the landing energy of the secondary electrons relative to the detection array, see paragraph [0135]). Regarding claim 5, Wieland discloses the charged particle optical device is configured to repel secondary signal particles emitted from the sample away from the down-beam array of detectors (controller configured to control potentials applied to the electrodes of the control lenses and the objective lenses to affect the landing energy of the secondary electrons relative to the detection array, see paragraph [0135]. The controller reduces landing energy by applying a potential to the electrodes to apply a repelling force to the secondary electrons. Any electrons below a certain energy level would be repelled.) Regarding claim 6, Wieland discloses the position of the down-beam array of detectors relative to the sample is selected to control detection of secondary signal particles by the down-beam array of detectors (interchangeable detector modules 240a-c may be interchangeable so that the detector module can be swapped between operable and non-operable positions between assessments of successive samples, see paragraphs [0146-0147]). Regarding claim 7, Wieland discloses the objective lens array comprises at least two electrodes in which are defined aperture arrays, corresponding apertures in the at least two electrodes are aligned with and arranged along a primary beam path, the at least two electrodes comprising an upper electrode and a lower electrode, the upper electrode being up-beam of the lower electrode along the primary beam path (objective lens 401 comprises an upper and lower electrode, aligned with one another to form a beam path to the sample 208, see Fig. 4). Regarding claim 8, Wieland discloses the down-beam array of detectors is associated with the lower electrode (detector module 402 located on the output side of the objective lens 401, see Fig. 4 and paragraph [0091]). Regarding claim 9, Wieland discloses the down-beam array of detectors is associated with a down-beam surface of the lower electrode (detector module 402 located on the output side of the objective lens 401, see Fig. 4 and paragraph [0091]; electron detection device is integrated with the lower electrode of an array objective lens, see paragraph [0121]). Regarding claim 10, Wieland discloses the up-beam array of detectors is associated with one of the at least two electrodes of the objective lens array (sensor units 503 may be integrated into or associated with the electrode of the objective lens 501 furthest from the sample 208, see paragraph [0121]). Regarding claim 11, Wieland discloses the up-beam array of detectors is associated with an up-beam surface of one of the at least two electrodes of the objective lens array, preferably wherein the up-beam array of detectors is associated with an up-beam surface of the (sensor units 503 may be integrated into or associated with the electrode of the objective lens 501 furthest from the sample 208, see paragraph [0121]). Regarding claim 12, Wieland discloses the up-beam array of detectors is associated with a down beam surface of one of the at least two electrodes of the objective lens array (sensor units may be positioned with the sensing surfaces located between the upbeam and downbeam facing surfaces of the upper electrodes, see paragraph [0121]). Regarding claim 13, Wieland discloses defined in each electrode are defined aperture arrays, desirably the objective lens array comprises at least two electrons in which are defined aperture arrays (objective lens 401 comprises an upper and lower electrode, aligned with one another to form a beam path through the array of apertures to the sample 208, see Fig. 4). Regarding claim 14, Wieland discloses each array of detectors comprises a plurality of detector elements around each beam aperture (detector modules 402 are formed around each beam aperture 406, see Figs. 4-6 and paragraph [0091]). Regarding claim 15, Wieland discloses a method of detecting charged particles emitted from a sample using a multi-beam charged particle assessment tool comprising the charged particle optical device (three sub-beams 311-313 are projected toward a sample 208, see paragraph [0070]; causing backscattered electrons to be released from the sample 208 which are detected by detector modules 402, see paragraph [0091]). Claim Rejections - 35 USC § 103 The following is a quotation of 35 U.S.C. 103 which forms the basis for all obviousness rejections set forth in this Office action: A patent for a claimed invention may not be obtained, notwithstanding that the claimed invention is not identically disclosed as set forth in section 102, if the differences between the claimed invention and the prior art are such that the claimed invention as a whole would have been obvious before the effective filing date of the claimed invention to a person having ordinary skill in the art to which the claimed invention pertains. Patentability shall not be negated by the manner in which the invention was made. Claim 2 is rejected under 35 U.S.C. 103 as being unpatentable over Wieland in view of Kruit et al. (US PGPub 2019/0259564, hereinafter Kruit). Regarding claim 2, Wieland discloses the up-beam array of detectors is arranged along the primary beam path (sensor unit 503 is mounted to the upper electrode of objective lens 501, see paragraph [0121]). Wieland fails to disclose the array of detectors is configured to face up-beam of the primary beam paths away from the sample. Kruit discloses a photo detector 130 directly above or on top of the electron to photon converter section 82 (e.g. facing away from the sample 11, see Fig. 13 and paragraph [0113]). Kuit modifies Wieland by suggesting providing the detectors on top of the electrodes to face away from the sample. Since both inventions are drawn to charged particle devices, it would have been obvious to the ordinary artisan before the effective filing date to modify Wieland by providing the detectors on top of the electrodes to face away from the sample for the purpose of minimizing the amount of components for a faster detection. Conclusion Any inquiry concerning this communication or earlier communications from the examiner should be directed to HANWAY CHANG whose telephone number is (571)270-5766. The examiner can normally be reached Monday - Friday 7:30 AM - 4:00 PM EST. Examiner interviews are available via telephone, in-person, and video conferencing using a USPTO supplied web-based collaboration tool. To schedule an interview, applicant is encouraged to use the USPTO Automated Interview Request (AIR) at http://www.uspto.gov/interviewpractice. If attempts to reach the examiner by telephone are unsuccessful, the examiner’s supervisor, Georgia Epps can be reached at (571) 272-2328. The fax phone number for the organization where this application or proceeding is assigned is 571-273-8300. Information regarding the status of published or unpublished applications may be obtained from Patent Center. Unpublished application information in Patent Center is available to registered users. To file and manage patent submissions in Patent Center, visit: https://patentcenter.uspto.gov. Visit https://www.uspto.gov/patents/apply/patent-center for more information about Patent Center and https://www.uspto.gov/patents/docx for information about filing in DOCX format. For additional questions, contact the Electronic Business Center (EBC) at 866-217-9197 (toll-free). If you would like assistance from a USPTO Customer Service Representative, call 800-786-9199 (IN USA OR CANADA) or 571-272-1000. Hanway Chang /HC/ Examiner, Art Unit 2878 /GEORGIA Y EPPS/ Supervisory Patent Examiner, Art Unit 2878
Read full office action

Prosecution Timeline

Nov 17, 2023
Application Filed
Jan 16, 2026
Non-Final Rejection — §102, §103 (current)

Precedent Cases

Applications granted by this same examiner with similar technology

Patent 12597582
Charged Particle Beam Apparatus
2y 5m to grant Granted Apr 07, 2026
Patent 12557588
METHODS OF CROSS-SECTION IMAGING OF AN INSPECTION VOLUME IN A WAFER
2y 5m to grant Granted Feb 17, 2026
Patent 12520413
SAPPHIRE LAMP FOR LASER SUSTAINED PLASMA BROADBAND LIGHT SOURCE
2y 5m to grant Granted Jan 06, 2026
Patent 12476073
SCANNING ELECTRON MICROSCOPE IMAGE-BASED PITCH WALK INSPECTION METHOD AND METHOD OF MANUFACTURING SEMICONDUCTOR DEVICE COMPRISING THE INSPECTION METHOD
2y 5m to grant Granted Nov 18, 2025
Patent 12463003
HIGH TEMPERATURE ION SOURCE
2y 5m to grant Granted Nov 04, 2025
Study what changed to get past this examiner. Based on 5 most recent grants.

AI Strategy Recommendation

Get an AI-powered prosecution strategy using examiner precedents, rejection analysis, and claim mapping.
Powered by AI — typically takes 5-10 seconds

Prosecution Projections

1-2
Expected OA Rounds
86%
Grant Probability
94%
With Interview (+7.6%)
2y 3m
Median Time to Grant
Low
PTA Risk
Based on 626 resolved cases by this examiner. Grant probability derived from career allow rate.

Sign in with your work email

Enter your email to receive a magic link. No password needed.

Personal email addresses (Gmail, Yahoo, etc.) are not accepted.

Free tier: 3 strategy analyses per month