Institute for Astrophysics and Computational Sciences
http://iacs.cua.edu

 
Richard D. Robinson


PERSONAL INFORMATION:

Position: Associate Research Professor, IACS, Catholic University of America
Address:   Code 681
  Goddard Space Flight Center
  Greenbelt, MD 20771
Office Location: Building 21, Room G33, Goddard Space Flight Center
Phone: (301) 286-4530
Fax: (301) 286-1752
E-mail : robinson@opal.gsfc.nasa.gov


RESEARCH INTERESTS:

I am primarily been involved in studies of the atmospheric physics of cool stars, particularly activity associated with magnetic fields. This includes the heating of chromospheres and coronae, the acceleration of winds, the dynamics of solar and stellar flares and the physical processes leading to starspots and prominances. I have been involved with the measurement of solar and stellar magnetic fields and am still interested in magnetic measurement techniques as well as the theory of the magnetic dynamo. Specific examples of current research topics are the following:

Winds in Cool Giant and Supergiant Stars:
Ken Carpenter and I have been analyzing GHRS spectra for a variety of cool giant and supergiant stars obtained from GTO and GO programs. The Fe II, Mg II and O I emission lines in these spectra show evidence for outwardly flowing material which increases in velocity with height, suggesting that we are observing the onset of the stellar wind in the chromosphere. I am currently using the SEI radiative transfer code (Sobolev with Exact Integration) to emperically model the winds in a few well observed stars, including the K giants alpha Tau and gamma Dra, the K supergiant lambda Vel and the M giant gamma Cru. This code was originally developed to investigate winds in hot stars, but has been found to provide excellent results in the investigation of cool stars as well. In most of the cool stars studied, the C II intercombination lines near 2330 \AA\ show significant non-thermal broadening with FWHM of $\sim$ 25 km s for the giants and $\sim$ 35 km s in the supergiants. This is highly supersonic and I am currently working with Vladimir Airapetian (CSC) and Leon Ofman (STX) on a model for atmospheric heating and wind acceleration based upon non-linear Alfven waves.

Flare Dynamics:
I have been collaborating with Bruce Woodgate in a search for proton beams during the impulsive phase of stellar flares. The original observations of the dMe flare star AU Mic consisted of rapid readout GHRS data obtained for Woodgate's HST GO program. These detected the signature of a proton beam. A second observation of AU Mic, taken approximately 1 year later, observed a small flare event which occurred during the decay phase of a much larger flare. No proton beam was detected, but a possible upper limit to the beam energy was obtained, as well as valuable information about the flare energy budget. A final set of observations were obtained for the star YZ CMi as part of a large observing campaign in Dec 1994. Approximately 29 flare events were detected during 7 hours of on-source observing. In nearly all cases the flares showed enhancements in both the lines and the continuum near 1200 \AA\ . Surprisingly, nearly all of the flares primarily showed low temperature enhancements, with little evidence for coronal emission. The continuum enhancements complicate the search for a proton beam signature and so far no evidence for proton beams have been seen. However, this may be expected based numerical simulations by Jeff Brosius (STX), which show that the lyman alpha emission from the proton beam may be rapidly suppressed by the ionization of the atmosphere.

Transition Regions and Coronae on Active Stars:
The Fe XXI line at 1354 \AA\ is the only coronal emission line currently available which can be resolved on a stellar source. Using observations obtained from Steve Maran's (NASA/LASP) HST GTO program, I have investigated the characteristics of the Fe XXI line on both the dMe flare star AU Mic and the RS CVn binary system HR 1099. The Fe XXI line was detected in both systems. The width of the line in AU Mic was consistent with a thermal plasma of temperature 10$^7$ K, which is the temperature where the ionization state is most pronounced. The observations for HR 1099 show emission from both components of the system, as well as a much broader width, suggesting either an extended corona or strong coronal turbulence. The O V line, seen in the same spectrum, is unresolved in the AU Mic observation, but is well resolved in the HR 1099 data and shows turbulent velocities with an RMS of more than 100 km s. Theoretical calculations by Airapetian (CSC) and myself indicate that the observations can be accounted for by the damping of non-linear Alfven waves in coronal loops. Apparently the heating processes occurring in the RS CVn and dMe stars are quite different.

Magnetic Activity on Hot Stars:

X-ray emission from hot stars is typically attributed to shock waves or the accretion of material onto a degenerate companion. The proto-typical Be star gamma Cas may be an exception to this rule. This star has an average X-ray emission which is much larger than typically seen in Be stars, but still an order of magnitude smaller than that seen in X-ray binaries. Myron Smith and I have been investigating the properties of the star and have found evidence that the X-rays may arise from flare-like activity near the stellar surface. These flares are seen as short duration (10-30 seconds) X-ray bursts superimposed on a slowly varying background. UV observations of the star taken with the Goddard High Resolution Spectrograph aboard the Hubble Space Telescope also show evidence for clouds of relatively cool plasma (5,000-20,000 K) which are suspended above the surface of the star and forced to co-rotate. These can be thought of as stellar analogs of solar prominences and, along with the flares, point to the presence of dynamic magnetic fields on this star.
 

Figure: 'GCAS_FULL_IMAGE.PS'

CAPTION: A dynamic UV spectrum of the classical Be star gamma Cas. The image represents a time sequence of spectra which have had an average reference spectrum subtracted so that spectral changes can be more easily observed. In all cases, the changes occur as absorption features. The color scale has been selected so that red corresponds to the maximum intensity (no absorption), while yellow, green, blue to white represent progressively larger amounts of absorption. The maximum absorption feature in the image corresponds to a decrease of about 20% below the local continuum intensity. The primary features result from blue-shifted absorption by the two resonance lines of Si IV (UV 1), which have rest wavelengths of 1393.73 Ang and 1402.73 Ang. These features have velocities of up to 1800 km/s and are often called Descrete Absorption Components (DACs). The dynamic spectrum is presented by Smith and Robinson (1999, ApJ, 517, 866) and a complete analysis of the DACs will be presented in an upcoming paper.
 


RESUME


PUBLICATIONS/ABSTRACTS: