Prosecution Insights
Last updated: April 19, 2026
Application No. 18/094,268

MODE-LOCKABLE RING OSCILLATOR AND ASSOCIATED METHODS

Non-Final OA §102
Filed
Jan 06, 2023
Examiner
PARK, KINAM
Art Unit
2828
Tech Center
2800 — Semiconductors & Electrical Systems
Assignee
Cornell University
OA Round
1 (Non-Final)
82%
Grant Probability
Favorable
1-2
OA Rounds
2y 6m
To Grant
89%
With Interview

Examiner Intelligence

Grants 82% — above average
82%
Career Allow Rate
680 granted / 829 resolved
+14.0% vs TC avg
Moderate +7% lift
Without
With
+7.3%
Interview Lift
resolved cases with interview
Typical timeline
2y 6m
Avg Prosecution
14 currently pending
Career history
843
Total Applications
across all art units

Statute-Specific Performance

§101
1.1%
-38.9% vs TC avg
§103
33.8%
-6.2% vs TC avg
§102
40.2%
+0.2% vs TC avg
§112
13.6%
-26.4% vs TC avg
Black line = Tech Center average estimate • Based on career data from 829 resolved cases

Office Action

§102
DETAILED ACTION 1. The present application, filed on or after March 16, 2013, is being examined under the first inventor to file provisions of the AIA . Claim Rejections - 35 USC § 102 2. 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. 3. Claims 1-20 are rejected under 35 U.S.C. 102(a)(1) as being anticipated by Wise et al. (US 20190305516). Regarding claim 9, Wise et al. discloses in figure 5 and specification: 9. A mode-lockable ring oscillator comprising: a gain element (see, Gain Fiber 1, fig. 5, see also, paragraph [0050]) that, when optically pumped (see, 976 nm Pump, fig. 5), amplifies an optical pulse into an amplified pulse; a gain-stage nonlinear optical element (see, paragraph [0050] ) configured to spectrally broaden the amplified pulse into a first spectrally-broadened pulse; a first optical filter (see, Filter 2, fig. 5) coupled to an output of the gain-stage nonlinear optical element, the first optical filter being configured to spectrally filter the first spectrally- broadened pulse into a first filtered pulse, the first optical filter having a first passband; a passive nonlinear optical element (see, paragraph [0050], here, passive SMF) coupled to an output of the first optical filter, the passive nonlinear optical element being configured to spectrally broaden the first filtered pulse into a second spectrally-broadened pulse; and a second optical filter (see, Gain Fiber 2, fig. 5) coupled to an output of the passive nonlinear optical element, the second optical filter being configured to filter the second spectrally-broadened pulse into a second filtered pulse, the second optical filter having a second passband that partially overlaps the first passband; wherein (i) an output of the second optical filter is coupled to an input of the gain element such that the gain element, gain-stage nonlinear optical element, first filter, passive nonlinear optical element, and second filter form a ring cavity and (ii) the mode-lockable ring oscillator is configured to initiate single-pulse mode-locking (see, paragraph [0043]). PNG media_image1.png 250 404 media_image1.png Greyscale Regarding claim 10, Wise et al. discloses in figure 5 and specification the mode-lockable ring oscillator of claim 9, the gain-stage nonlinear optical element being configured such that a spectrum of the first spectrally-broadened pulse exceeds a bandwidth of an emission cross-section of the gain element (see, paragraph [0056]). Regarding claim 11, Wise et al. discloses in figure 5 and specification the mode-lockable ring oscillator of claim 9, the gain element and the gain-stage nonlinear optical element comprising the same optical element (see, paragraph [0050]). Regarding claim 12, Wise et al. discloses in figure 5 and specification the mode-lockable ring oscillator of claim 11, the same optical element comprising a doped optical fiber (see, paragraph [0050]). Regarding claim 13, Wise et al. discloses in figure 5 and specification the mode-lockable ring oscillator of claim 12, the doped optical fiber being polarization- maintaining (see, paragraph [0045]). Regarding claim 14, Wise et al. discloses in figure 5 and specification the mode-lockable ring oscillator of claim 12, the doped optical fiber comprising a large- mode-area optical fiber, a photonic-crystal fiber, or a microstructure fiber, or a combination thereof (see, paragraph [0041]). Regarding claim 15, Wise et al. discloses in figure 5 and specification the mode-lockable ring oscillator of claim 9, configured to amplify the optical pulse in the gain element with gain-managed nonlinearity(see, paragraph [0041]). Regarding claim 16, Wise et al. discloses in figure 5 and specification the mode-lockable ring oscillator of claim 9, the passive nonlinear optical element comprising a passive optical fiber(see, paragraph [0050]). Regarding claim 17, Wise et al. discloses in figure 5 and specification the mode-lockable ring oscillator of claim 16, the passive optical fiber being polarization-maintaining (see, paragraph [0045]). Regarding claim 18, Wise et al. discloses in figure 5 and specification the mode-lockable ring oscillator of claim 9, the first filter comprising a rejection port from which spectral components rejected by the first filter are coupled out of the ring cavity (see, paragraph [0050]). Regarding claim 19, Wise et al. discloses in figure 5 and specification the mode-lockable ring oscillator of claim 12, consisting of only polarization- maintaining fiber-optic-based components (see, paragraph [0045]). Regarding claim 20, Wise et al. discloses in figure 5 and specification a method comprising: pumping the gain element of the mode-lockable ring oscillator of claim 9 with pump light; modulating the pump light during said pumping to initiate single-pulse mode-locking of the mode-lockable ring oscillator, wherein the second passband of the second optical filter partially overlaps the first passband of the first filter when the single- pulse mode-locking is initiated; and stopping said modulating after the mode-lockable ring oscillator has initiated single-pulse mode-locking. (see, paragraph [0050]) Regarding claims 1-8, method claims 1-8 are rejected for the same reasons applied to device claims 9-20 since the limitations of method claims 1-8 are implemented by the limitations of devices claims 9-20. Conclusion 4. Any inquiry concerning this communication or earlier communications from the examiner should be directed to Kinam Park whose telephone number is (571) 270-1738. The examiner can normally be reached on from 9:00 AM-5:00 PM. If attempts to reach the examiner by telephone are unsuccessful, the examiner's supervisor, MINSUN HARVEY, can be reached on (571) 272-1835. The fax phone number for the organization where this application or proceeding is assigned is 571-273-8300. Information regarding the status of an application may be obtained from the Patent Application Information Retrieval (PAIR) system. Status information for published applications may be obtained from either Private PAIR or Public PAIR. Status information for unpublished applications is available through Private PAIR only. For more information about the PAIR system, see http://pair-direct.uspto.gov. Should you have questions on access to the Private PAIR system, contact the Electronic Business Center (EBC) at 866-217-9197 (toll-free). /KINAM PARK/Primary Examiner, Art Unit 2828
Read full office action

Prosecution Timeline

Jan 06, 2023
Application Filed
Jan 10, 2026
Non-Final Rejection — §102 (current)

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Study what changed to get past this examiner. Based on 5 most recent grants.

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Prosecution Projections

1-2
Expected OA Rounds
82%
Grant Probability
89%
With Interview (+7.3%)
2y 6m
Median Time to Grant
Low
PTA Risk
Based on 829 resolved cases by this examiner. Grant probability derived from career allow rate.

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