Prosecution Insights
Last updated: October 01, 2026
Application No. 18/636,334

Magnetometer Array System For Magnetically Noisy Environments

Non-Final OA §112
Filed
Apr 16, 2024
Priority
Apr 24, 2023 — provisional 63/461,359
Examiner
KUAN, JOHN CHUNYANG
Art Unit
Tech Center
Assignee
The Regents of the University of Michigan
OA Round
1 (Non-Final)
72%
Grant Probability
Favorable
1-2
OA Rounds
7m
Est. Remaining
99%
With Interview

Examiner Intelligence

Grants 72% — above average
72%
Career Allowance Rate
407 granted / 563 resolved
+12.3% vs TC avg
Strong +48% interview lift
Without
With
+47.6%
Interview Lift
resolved cases with interview
Typical timeline
3y 0m
Avg Prosecution
32 currently pending
Career history
587
Total Applications
across all art units

Statute-Specific Performance

§101
28.1%
-11.9% vs TC avg
§103
32.6%
-7.4% vs TC avg
§102
9.3%
-30.7% vs TC avg
§112
24.9%
-15.1% vs TC avg
Black line = Tech Center average estimate • Based on career data from 563 resolved cases

Office Action

§112
DETAILED ACTION Notice of Pre-AIA or AIA Status The present application, filed on or after March 16, 2013, is being examined under the first inventor to file provisions of the AIA . Specification The disclosure is objected to because of the following informalities: In [0087], line 8, “Fifth (e)” should be --Fifth (v)-- to be consistent in the numbering scheme and be consistent with FIG. 4. Appropriate correction is required. Claim Objections Claims 1-11 are objected to because of the following informalities: In claim 1, line 5, “magnetic noise and geomagnetic field data” should be --the magnetic noise and the geomagnetic field data-- to void creating another antecedent bases (see the preamble for the antecedent bases). In claim 1, line 8, “the magnetic noise data” should be --the magnetic noise-- to avoid the issue of lack of antecedent basis. In claim 5, lines 2-3, “the magnetic noise data” should be --the magnetic noise-- to avoid the issue of lack of antecedent basis. In claim 6, line 5, “magnetic noise and geomagnetic field data” should be --the magnetic noise and the geomagnetic field data-- to void creating another antecedent bases (see the preamble for the antecedent bases). In claim 6, lines 7-8, “the magnetic noise data” should be --the magnetic noise-- to avoid the issue of lack of antecedent basis. In claim 11, line 3, “the magnetic noise data” should be --the magnetic noise-- to avoid the issue of lack of antecedent basis. The other claim(s) not discussed above, or depending on the above claim(s), are objected to for inheriting the issue(s) from their linking claim(s). Appropriate correction is required. Claim Rejections - 35 USC § 112 The following is a quotation of 35 U.S.C. 112(b): (b) CONCLUSION.—The specification shall conclude with one or more claims particularly pointing out and distinctly claiming the subject matter which the inventor or a joint inventor regards as the invention. The following is a quotation of 35 U.S.C. 112 (pre-AIA ), second paragraph: The specification shall conclude with one or more claims particularly pointing out and distinctly claiming the subject matter which the applicant regards as his invention. Claims 1-11 are rejected under 35 U.S.C. 112(b) or 35 U.S.C. 112 (pre-AIA ), second paragraph, as being indefinite for failing to particularly point out and distinctly claim the subject matter which the inventor or a joint inventor (or for applications subject to pre-AIA 35 U.S.C. 112, the applicant), regards as the invention. Regarding claim 1, it recites “analyzing a relative gain and phase of the representative detection signal in a time-frequency (TF) domain, if a noise signal of the representative detection signal is sparse in the TF domain then the relative gain and phase is found using cluster analysis” in lines 9-12. It appears that finding the relative gain and phase is contingent on a noise signal of the representative detection signal being sparse in the TF domain. However, it is unclear whether “analyzing a relative gain and phase of the representative detection signal in a time-frequency (TF) domain” is also contingent on a noise signal of the representative detection signal being sparse in the TF domain. For examination purpose, --analyzing a relative gain and phase of the representative detection signal in a time-frequency (TF) domain, [[if]]wherein a noise signal of the representative detection signal is sparse in the TF domain and the relative gain and phase is found using cluster analysis-- is assumed. In claim 5, it recites “each axis of the plurality of magnetometers” in lines 3-4. It is unclear whether it means “an axis of each of the plurality of magnetometers”, “each of a plurality of axes of the plurality of magnetometers”, or else. For examination purpose, --an axis of each of the plurality of magnetometers-- is assumed. Regarding claim 6, it recites “analyzing a relative gain and phase of the representative detection signal in a time-frequency (TF) domain, if a noise signal of the representative detection signal is sparse in the TF domain then the relative gain and phase is found using cluster analysis” in lines 9-12. It appears that finding the relative gain and phase is contingent on a noise signal of the representative detection signal being sparse in the TF domain. However, it is unclear whether “analyzing a relative gain and phase of the representative detection signal in a time-frequency (TF) domain” is also contingent on a noise signal of the representative detection signal being sparse in the TF domain. For examination purpose, --analyzing a relative gain and phase of the representative detection signal in a time-frequency (TF) domain, [[if]]wherein a noise signal of the representative detection signal is sparse in the TF domain and the relative gain and phase is found using cluster analysis-- is assumed. In claim 11, it recites “each axis of the plurality of magnetometers” in lines 4-5. It is unclear whether it means “an axis of each of the plurality of magnetometers”, “each of a plurality of axes of the plurality of magnetometers”, or else. For examination purpose, --an axis of each of the plurality of magnetometers-- is assumed. The other claim(s) not discussed above, or depending on the above claim(s), are rejected for inheriting the issue(s) from their linking claim(s). Notes Claims 1 and 6 distinguish over the closest prior art of record as discussed below. Regarding claims 1 and 6, the closest prior art of record fails to teach the feature of claim 1 (as the representative): “analyzing a relative gain and phase of the representative detection signal in a time-frequency (TF) domain, if a noise signal of the representative detection signal is sparse in the TF domain then the relative gain and phase is found using cluster analysis, and separating a geomagnetic field data signal from a magnetic noise data signal using cluster centroids in compressive sensing based on the cluster analysis,” in combination with the rest of the claim limitations as claimed and defined by the Applicant. The method separates the noise signal by clustering data in TF domain and performing compressive sensing. Carter et al. ("CORRECTING GOES-R MAGNETOMETER DATA FOR STRAY FIELDS" 2016 ESA Workshop on Aerospace EMC (Aerospace EMC), Valencia, Spain, 2016) teaches a method of separating stray magnetic noise from geomagnetic field data by using an algorithm to switch between using gradiometry or averaging measurements of magnetometers. Ream et al. ("Magnetic gradiometry using frequency-domain filtering" Meas. Sci. Technol. 33 (2022) 015104; cited in IDS) teaches a gradiometry algorithm that detects stray magnetic field signals through differencing magnetometer measurements in the time-domain and suppressing them in the frequency-domain. Constantinescu et al. ("Maximum-variance gradiometer technique for removal of spacecraft-generated disturbances from magnetic field data" Geosci. Instrum. Method. Data Syst., 9, 451-469, 2020) teaches an algorithm that transforms a dual-magnetometer measurements into a new coordinate system derived from principle component analysis, and performs gradiometry along the direction of maximum-variance. SHEINKER et al. ("Adaptive Interference Cancelation Using a Pair of Magnetometers" IEEE TRANSACTIONS ON AEROSPACE AND ELECTRONIC SYSTEMS VOL. 52, NO. 1 FEBRUARY 2016) teaches an analytical blind source separation method to remove a single noise source using a pair of magnetometers. Imajo et al. ("Signal and Noise Separation From Satellite Magnetic Field Data Through Independent Component Analysis: Prospect of Magnetic Measurements Without Boom and Noise Source Information" Journal of Geophysical Research: Space Physics, 126, e2020JA028790, 2021; cited in IDS) teaches a noise separation method by applying Independent Component Analysis to separate noise signal based on their statistical independence. The above are the closest references that utilize two or more magnetometers to facilitate the separation of the noise signal. Still, none of the prior art of record teaches or suggests the above indicated feature as claimed. Prior Art The prior art made of record and not relied upon is considered pertinent to applicant's disclosure. ZHU et al. (CN 110673206 A) teaches a satellite magnetic field data seismic abnormality detection method, involving decomposing magnetic field in time-frequency domain to separate components caused by earthquake and components caused by solar activity. ZHANG et al. (CN 106842344 B) teaches a unmanned aerial vehicle navigation magnetic full-axis gradient magnetic interference compensation method, involving training a feedforward networking to take normalized wavelet transformation of flight magnetic data as input, and output magnetic interference compensation data; and compensating the magnetic field measurement using the compensation data. KIM et al. (US 20180115874 A1) teaches a method for performing geomagnetic signal processing, involving converting obtained geomagnetic signal into a high frequency signal using a signal processing filter; extracting abnormal high frequency signal values; determining whether a sum of the extracted abnormal high frequency signal values converges into a critical range a preset time window; and correcting the geomagnetic signal based on the determining. Conclusion Any inquiry concerning this communication or earlier communications from the examiner should be directed to JOHN C KUAN whose telephone number is (571)270-7066. The examiner can normally be reached M-F: 9:00AM-5:30PM. 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, Andrew Schechter can be reached at (571) 272-2302. 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. /JOHN C KUAN/Primary Examiner, Art Unit 2857
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Prosecution Timeline

Apr 16, 2024
Application Filed
Aug 12, 2026
Non-Final Rejection mailed — §112 (current)

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Prosecution Projections

1-2
Expected OA Rounds
72%
Grant Probability
99%
With Interview (+47.6%)
3y 0m (~7m remaining)
Median Time to Grant
Low
PTA Risk
Based on 563 resolved cases by this examiner. Grant probability derived from career allowance rate.

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