I was born in Taipei City, Taiwan. Since childhood, I have been fascinated by the beauty of the natural sciences, which inspired me to pursue a B.S. degree in Earth Sciences. In my sophomore year, I was first introduced to professional astronomy research, which led me to complete an M.S. degree in Astronomy at National Taiwan Normal University and a Ph.D. in Astrophysics at Ludwig-Maximilians-Universität München. I am now eager to further explore various aspects of astronomy, including both software and hardware development. My personal interests include watching operas, musicals, and Japanese animation.
Ming-Yi LIN
University of Toledo
2801 Bancroft St, Toledo,
Ohio, 43606, USA
- Keck
I am currently working on the NSF-funded AGN project (PI: Prof. Anne Medling). My work focuses on analyzing OSIRIS data, including improving the mosaics and studying the gas and stellar kinematics. I plan to build a dynamical mass model to test the modified Bondi SMBH accretion as well as accretion driven by gravitational torques.
- Very Large Telescope (VLT)
The VLT Large Program (PI: Dr. Richard Davies) goes into individual ESO observation period (93P, 98P, and 99P). My works include preparing the observation blocks (OBs), doing the data reduction, and improving the calibration pipeline. In order to retrieve higher S/N ratio in absorption lines, I reduce the effects of differential atmospheric refraction by theoretical calculation in the both the image and spectroscopy. Such effect becomes significant for high-resolution observations (e.g. AO mode) at near-infrared wavelengths.
- Institut de Radioastronomie Millimétrique (IRAM)
I studied HCN and HCO⁺ emission in the nuclear regions of nearby AGNs using data from the Plateau de Bure Interferometer (PdBI). Recently, I have been using the new NOEMA-PolyFix instrument to observe CO gas kinematics and investigate AGN feedback mechanisms.
- Yuan-Tseh Lee Array (YTLA)
It is a 7 small dishes interferometer project leaded by Taiwan (former name:AMiBA). I assist daytime and nighttime observing and work closely with engineers/project scientist to do the troubleshooting, for example: decompose the antennae amplitudes and looking for whether they correlate to the instrumental temperatures. I also measure the quasar continuum flux density, then compare to the System Equivalent Flux Density (SEFD) in order to check the instrument stability, it is a part of commissioning test and verification phases. (On site during Aug 2018, Oct-Dec 2018).
- Submillimeter Array (SMA)
My first professional astronomy research is using SMA data to study the shell kinematics of post-AGB star. I used MIR and MIRID to flag out bad data and reconstruct the image. I also complete one night observation for the summer student group project – searching the methanol signal from high-z galaxy.
- Binocular Telescope (LBT)
The science program belongs to Dr. Eva Wuyts. I was a volunteer student to work with instrument scientists and telescope operators. In the six-day observations, my works included assisting the observing program execution, assessing weather condition, communicating with LBTO staff.
Distribution of XMM and Chandra indicate these samples are drawn from the same population. However, the distribution of 70μm/X-ray sample and X-ray selected samples seem not to be drawn from the same population. The distributions indicate an excess of HR ≥ -0.3, revealing that the cold dust from the host galaxy may be responsible for additional obscuration.
We use dense molecular gas HCN(1-0) and HCO+(1-0) at 1” resolution to trace the rotating molecular disk on scales of ~100 pc scale for nearby Seyferts. By modeling the observed kinematics, we find that the geometrically think molecular disk is quite common, indicating the supernovae could potentially being a source to provide the additional energy to maintain the vertical structure.
The best sample of simple toy model to explain the trend of radial stellar velocity dispersion. Top panel: The radial luminosity for observed data point (black pluses) and bulge component (red dashed line). Middle panel: The bulge fraction as a function of radius. Bottom panel: The radial stellar velocity dispersion with radius. The black solid line represents the intrinsic bulge velocity dispersion, which is calculated based on the bulge surface brightness prole. Considering the contributions come from both a dynamically hot bulge population (typical is several hundredkm/s) and a dynamically cold young star population (we assume 40-50 km/s), the luminosity-weighted velocity dispersion is presented in blue dashed line. Pink pluses are the observed data with the error bar representing the 1-σ error with respect to the velocity dispersion inside the 2-D elliptical rings at specic radius. We attached the pPXF return mean stellar velocity dispersion error (25km/s in average) in the bottom left corner.
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