General Motors
Lead Digital 3D Designer
Gm Patac
Lead Creative Design Sculptor
Gm Advance Design Studio Aug 2012 - Jul 2015
Lead 3D Designer
General Motors Aug 2012 - Jul 2015
3D Design Sculptor
Education:
Academy of Art University 2005 - 2009
Skills:
Product Design Alias Studio Tools Industrial Design Concept Design Concept Development Automotive Design Sketching Rendering Automotive Design Strategy Cad Design Thinking Rapid Prototyping Illustrator
Anatoliy A. Savchenkov - Glendale CA, US Nan Yu - Arcadia CA, US Lute Maleki - Pasadena CA, US Vladimir S. Iltchenko - Arcadia CA, US Andrey B. Matsko - Pasadena CA, US Dmitry V. Strekalov - Arcadia CA, US
Assignee:
The United States of America as represented by the Administrator of the National Aeronautics and Space Administration - Washington DC
International Classification:
G01K 11/26 G01K 1/00 G01H 1/14 G01H 3/04
US Classification:
374117, 374130, 374127, 374120, 73579, 382 28
Abstract:
A differential temperature sensor system and method of determining a temperature shift of an optical resonator and its surroundings are provided. The differential temperature sensor system includes a light generating device capable of generating a beam having a carrier frequency, a modulator capable of modulating the beam with a sideband frequency, and an optical resonator capable of supporting an ordinary mode and an extraordinary mode. The system includes an ordinary mode-lock setup capable of locking the carrier frequency of the beam to the ordinary mode of the optical resonator and an extraordinary mode-lock setup capable of locking the sideband frequency of the beam to the extraordinary mode of the optical resonator by providing a specific radio frequency to the modulator substantially corresponding to a frequency shift between the ordinary mode and the extraordinary mode of the optical resonator resulting from a temperature change of the optical resonator. A processor precisely calculates the differential temperature based upon the frequency shift between the ordinary mode and extraordinary mode of the optical resonator.
Optical Sensing Based On Overlapping Optical Modes In Optical Resonator Sensors And Interferometric Sensors
Thanh M. Le - Duarte CA, US Nan Yu - Arcadia CA, US Anatoliy Savchenkov - Glendale CA, US William H. Steier - San Marino CA, US
Assignee:
OEwaves, Inc. - Pasadena CA California Institute of Technology - Pasadena CA University of Southern California - Los Angeles CA
International Classification:
G01B 9/02
US Classification:
356491, 356480
Abstract:
Techniques and devices based on transverse magnetic (TM) and transverse electric (TE) modes in an optical resonator or interferometer to provide sensitive optical detection with insensitivity to a change in temperature. A shift in a difference between a first resonance wavelength of a TE optical mode and a second resonance wavelength of a TM optical mode is measured to measure a change in a sample that is in optical interaction with the optical resonator or interferometer. For example, the detected shift can be used to measure a change in a refractive index of the sample.
Nan Yu - Arcadia CA, US Andrey B. Matsko - Pasadena CA, US Anatoliy Savchenkov - Glendale CA, US
Assignee:
California Institute of Technology - Pasadena CA
International Classification:
G01N 29/24 G01N 29/46
US Classification:
73643
Abstract:
Designs of single-beam laser vibrometry systems and methods. For example, a method for detecting vibrations of a target based on optical sensing is provided to include operating a laser to produce a laser probe beam at a laser frequency and modulated at a modulation frequency onto a target; collecting light at or near the laser to collect light from the target while the target is being illuminated by the laser probe beam through an optical receiver aperture; using a narrow-band optical filter centered at the laser frequency to filter light collected from the optical receiver aperture to transmit light at the laser frequency while blocking light at other frequencies; using an optical detector to convert filtered light from the narrow-band optical filter to produce a receiver electrical signal; using a lock-in amplifier to detect and amplify the receiver electrical signal at the modulation frequency while rejecting signal components at other frequencies to produce an amplified receiver electrical signal; processing the amplified receiver electrical signal to extract information on vibrations of the target carried by reflected laser probe beam in the collected light; and controlling optical power of the laser probe beam at the target to follow optical power of background illumination at the target.
Atomic Clock Based On An Opto-Electronic Oscillator
Opto-electronic oscillators having a frequency locking mechanism to stabilize the oscillation frequency of the oscillators to an atomic frequency reference. Whispering gallery mode optical resonators may be used in such oscillators to form compact atomic clocks.
Method Of Engineering The Dispersion Of Whispering Gallery Mode Resonators And The Resonators With Dispersion Engineered By The Method
- Pasadena CA, US Nan Yu - Arcadia CA, US Lukas M. Baumgartel - Portland OR, US
International Classification:
G02B 6/293 G06F 17/13 G02B 27/00
Abstract:
A method for fabricating a resonator structure, comprising engineering dispersion of electromagnetic radiation guided along a boundary of an axially symmetric substrate, the engineering comprising micro-structuring a geometry of the boundary, wherein the structure defines a waveguide for electromagnetic radiation.
Point-Wise Phase Matching For Nonlinear Frequency Generation In Dielectric Resonators
Nan Yu - Arcadia CA, US Dmitry V. Strekalov - Arcadia CA, US Guoping Lin - Pasadena CA, US
Assignee:
CALIFORNIA INSTITUTE OF TECHNOLOGY - Pasadena CA
International Classification:
G02F 1/37 G02F 1/355 G02F 1/35
US Classification:
359328
Abstract:
An optical resonator fabricated from a uniaxial birefringent crystal, such as beta barium borate. The crystal is cut with the optical axis not perpendicular to a face of the cut crystal. In some cases the optical axis lies in the plane of the cut crystal face. An incident (input) electromagnetic signal (which can range from the infrared through the visible to the ultraviolet) is applied to the resonator. An output signal is recovered which has a frequency that is an integer multiple of the frequency of the input signal. In some cases a prism is used to evanescently couple the input and the output signals to the resonator.