Department of Financial Engineering Yong'An, CN Jan 2009 to Sep 2014 DirectorUnis Tianhe Co., LTD
Apr 2004 to Apr 2005 Software Developer
Education:
Peking University 2005 to 2009 Master of Science in PhysicsPeking University 1999 to 2003 Bachelor of Science in Physics, Computer
Skills:
- Advanced Statistics, Time Series Analysis, Mathematical Modeling<br/>- Data Processing, Data Mining, Machine learning, Big Data<br/>- C++, Java, Python, Matlab, MySQL<br/>- Operating Systems: Windows, Linux
2011 to 2000 Senior Analyst Schedule PlanningFEDERAL AVIATION ADMINSTRATION (FAA) Washington, DC 2006 to 2011 Operation Research AnalystNATIONAL CENTER OF EXCELLENCE FOR AVIATION OPERATIONS RESEARCH (NEXTOR) Berkeley, CA 2005 to 2006 Graduate Research Assistant
Education:
NEW YORK UNIVERSITY New York, NY Jan 2015 Master of Business Administration in SpecializationsUNIVERSITY OF CALIFORNIA, BERKELEY Berkeley, CA Jun 2014UC Berkeley 2001
Timothy R. Piwonka-Corle - Portland OR Karen F. Scoffone - Redwood City CA Xing Chen - San Jose CA Jean-Louis Stehle - Colombes, FR Dorian Zahorski - Vanves, FR John-Pierre Rey - Fontenay Aux Roses, FR
Assignee:
KLA-Tencor Technologies Corporation - Milpitas CA
International Classification:
G01N 2121
US Classification:
356369
Abstract:
A method and system for spectroscopic ellipsometry employing reflective optics to measure a small region of a sample by reflecting radiation (preferably broadband UV, visible, and near infrared radiation) from the region. The system preferably has an autofocus assembly and a processor programmed to determine from the measurements the thickness and/or complex refractive index of a thin film on the sample. Preferably, only reflective optics are employed along the optical path between the polarizer and analyzer, a sample beam reflects with low incidence angle from each component of the reflective optics, the beam is reflectively focused to a small, compact spot on the sample at a range of high incidence angles, and an incidence angle selection element is provided for selecting for measurement only radiation reflected from the sample at a single, selected angle (or narrow range of angles). The focusing mirror preferably has an elliptical shape to reduce off-axis aberrations in the focused beam. Some embodiments include both a spectrophotometer and an ellipsometer integrated together as a single instrument.
Optical Interleaving With Enhanced Spectral Response And Reduced Polarization Sensitivity
Hwan J. Jeong - Los Altos CA, US Xing Chen - San Jose CA, US
Assignee:
Gazillion Bits, Inc. - San Jose CA
International Classification:
G20B006/42
US Classification:
385 39, 385 24, 359497, 398 82
Abstract:
An optical interleaver is described, comprising a splitting element for splitting an incident beam into a first optical signal directed along a first path and a second optical signal directed along a second path, a first resonant element positioned along the first path, a second resonant element positioned along the second path, and a combining element positioned to receive and to interferometrically combine the outputs of the first and second resonant to produce the output signal. The optical interleaver may be implemented using a free-space configuration using a beamsplitter and a plurality of resonant cavities such as asymmetric Fabry-Perot resonators or Michelson-Gires-Tournois resonators. In an alternative preferred embodiment, the optical interleaver may be implemented in a Mach-Zender-style configuration using couplers and fiber ring resonators.
Chemical Ionization Reaction Or Proton Transfer Reaction Mass Spectrometry With A Quadrupole Mass Spectrometer
Timothy Roger Robinson - Burland, GB Mark Attwood - Cupertino CA, US Xing Chen - Lexington MA, US William M. Holber - Winchester MA, US Mark Philip Longson - Waterhouses, GB Jonathan Henry Palk - Sandbach, GB Ali Shajii - Canton MA, US John A. Smith - North Andover MA, US
Assignee:
MKS Instruments, Inc. - Andover MA
International Classification:
H01J 49/26
US Classification:
250288, 250281, 250282, 250283, 250423 R, 250424
Abstract:
A system and methods are described for generating reagent ions and product ions for use in a quadruple mass spectrometry system. A microwave or high-frequency RF energy source ionizes particles of a reagent vapor to form reagent ions. The reagent ions enter a chamber, such as a drift chamber, to interact with a fluid sample. An electric field directs the reagent ions and facilitates an interaction with the fluid sample to form product ions. The reagent ions and product ions then exit the chamber under the influence of an electric field for detection by a quadruple mass spectrometer module. The system includes various control modules for setting values of system parameters and analysis modules for detection of mass values for ion species during spectrometry and faults within the system.
Chemical Ionization Reaction Or Proton Transfer Reaction Mass Spectrometry With A Time-Of-Flight Mass Spectrometer
Timothy Roger Robinson - Burland, GB Mark Attwood - Cupertino CA, US Xing Chen - Lexington MA, US William M. Holber - Winchester MA, US Mark Philip Longson - Waterhouses, GB Jonathan Henry Palk - Sandbach, GB Ali Shajii - Canton MA, US John A. Smith - North Andover MA, US
Assignee:
MKS Instruments, Inc. - Andover MA
International Classification:
H01J 49/26
US Classification:
250288, 250281, 250282, 250283, 250423 R, 250424
Abstract:
A system, components thereof, and methods are described for time-of-flight mass spectrometry. A microwave or high-frequency RF energy source is used to ionize a reagent vapor to form reagent ions. The reagent ions enter a chamber and interact with a fluid sample to form product ions. The reagent ions and product ions are directed to a time-of-flight mass spectrometer module for detection and determination of a mass value for the ions. The time-of-flight mass spectrometer module can include an optical system and an ion beam adjuster for focusing, interrupting, or altering a flow of reagent and product ions according to a specified pattern. The time-of-flight mass spectrometer module can include signal processing techniques to collect and analyze an acquired signal, for example, using statistical signal processing, such as maximum likelihood signal processing.
Chemical Ionization Reaction Or Proton Transfer Reaction Mass Spectrometry
Timothy Roger Robinson - Burland, GB Mark Attwood - Cupertino CA, US Xing Chen - Lexington MA, US William M. Holber - Winchester MA, US Mark Philip Longson - Waterhouses, GB Jonathan Henry Palk - Sandbach, GB Ali Shajii - Canton MA, US John A. Smith - North Andover MA, US
Assignee:
MKS Instruments, Inc. - Andover MA
International Classification:
H01J 49/26
US Classification:
250288, 250281, 250282, 250283, 250423 R, 250424
Abstract:
A system and methods are described for generating reagent ions and product ions for use in a mass spectrometry system. Applications for the system and method are also disclosed for detecting volatile organic compounds in trace concentrations. A microwave or high-frequency RF energy source ionizes particles of a reagent vapor to form reagent ions. The reagent ions enter a chamber, such as a drift chamber, to interact with a fluid sample. An electric field directs the reagent ions and facilitates an interaction with the fluid sample to form product ions. The reagent ions and product ions then exit the chamber under the influence of an electric field for detection by a mass spectrometer module. The system includes various control modules for setting values of system parameters and analysis modules for detection of mass and peak intensity values for ion species during spectrometry and faults within the system.
Focused Beam Spectroscopic Ellipsometry Method And System
Timothy Piwonka-Corle - Portland OR, US Karen Scoffone - Redwood City CA, US Xing Chen - San Jose CA, US Lloyd Lacomb - Santa Clara CA, US Jean-Louis Stehle - Colombes, FR Dorian Zahorski - Vanves, FR Jean-Pierre Rey - Fontenay Aux Roses, FR
International Classification:
G01J004/00
US Classification:
356/364000
Abstract:
A method and system for spectroscopic ellipsometry employing reflective optics to measure a small region of a sample by reflecting radiation (preferably broadband UV, visible, and near infrared radiation) from the region. The system preferably has an autofocus assembly and a processor programmed to determine from the measurements the thickness and/or complex refractive index of a thin film on the sample. Preferably, only reflective optics are employed along the optical path between the polarizer and analyzer, a sample beam reflects with low incidence angle from each component of the reflective optics, the beam is reflectively focused to a small, compact spot on the sample at a range of high incidence angles, and an incidence angle selection element is provided for selecting for measurement only radiation reflected from the sample at a single, selected angle (or narrow range of angles). The focusing mirror preferably has an elliptical shape to reduce off-axis aberrations in the focused beam. Some embodiments include both a spectrophotometer and an ellipsometer integrated together as a single instrument. In such instrument, the spectrophotometer and ellipsometer share a radiation source, and radiation from the source can be focused by either the spectrophotometer or the ellipsometer to the same focal point on a sample. Preferred embodiments of the ellipsometer employ a rotating, minimal-length Rochon prism as a polarizer, and include a spectrometer with an intensified photodiode array to measure reflected radiation from the sample, and a reference channel (in addition to a sample channel which detects radiation reflected from the sample).
Focused Beam Spectroscopic Ellipsometry Method And System
Timothy Piwonka-Corle - Portland OR, US Karen Scoffone - Redwood City CA, US Xing Chen - San Jose CA, US Lloyd Lacomb - Santa Clara CA, US Jean-Louis Stehle - Colombes, FR Dorian Zahorski - Vanves, FR John-Pierre Rey - Fontenay Aux Roses, FR
International Classification:
G01J004/00
US Classification:
356369000
Abstract:
A method and system for spectroscopic ellipsometry employing reflective optics to measure a small region of a sample by reflecting radiation (preferably broadband UV, visible, and near infrared radiation) from the region. The system preferably has an autofocus assembly and a processor programmed to determine from the measurements the thickness and/or complex refractive index of a thin film on the sample. Preferably, only reflective optics are employed along the optical path between the polarizer and analyzer, a sample beam reflects with low incidence angle from each component of the reflective optics, the beam is reflectively focused to a small, compact spot on the sample at a range of high incidence angles, and an incidence angle selection element is provided for selecting for measurement only radiation reflected from the sample at a single, selected angle (or narrow range of angles). The focusing mirror preferably has an elliptical shape to reduce off-axis aberrations in the focused beam. Some embodiments include both a spectrophotometer and an ellipsometer integrated together as a single instrument. In such instrument, the spectrophotometer and ellipsometer share a radiation source, and radiation from the source can be focused by either the spectrophotometer or the ellipsometer to the same focal point on a sample. Preferred embodiments of the ellipsometer employ a rotating, minimal-length Rochon prism as a polarizer, and include a spectrometer with an intensified photodiode array to measure reflected radiation from the sample, and a reference channel (in addition to a sample channel which detects radiation reflected from the sample).
Joseph Carter - San Jose CA Jennming Chen - Campbell CA Xing Chen - San Jose CA
Assignee:
Kla-Tencor Corporation - San Jose CA
International Classification:
G01J 336 G01N 2121
US Classification:
356326
Abstract:
The pixel position-to-wavelength calibration function of film measurement devices such as spectroscopic ellipsometers and spectroreflectometers may shift due to temperature and humidity changes and mechanical factors. One or more wavelength markers provided by the light source or reference sample may be used to correct the calibration function. The pixel positions of one or more persistent wavelength markers are noted during the calibration process and the current positions of such markers are again noted to account for shifts due to various factors to correct the calibration function.