My group from Williams College,
including my colleague Bryce Babcock and 8 students, successfully observed the
annular eclipse from the National Radio Astronomy Observatory's Jansky Very Large Array, sixty miles west of Socorro New
Mexico. I was working with Dale Gary of the New Jersey Institute of
Technology, Tim Bastian of NRAO, and Stephen White of Air Force Research
Laboratory to make high-resolution radio observations of the annular eclipse
with the JVLA and with the CARMA array in the Inyo Mountains of California.
I was also working with Dr. Thomas Kuiper of
JPL on using the 34-m Goldstone antenna, also to get high-resolution solar
observations as the advancing edge of the moon defined the time and position on
the Sun of solar active regions as seen in the radio, improving on capabilities
outside of eclipse. Our observations were successful, and it will take
months to analyze the data.
Jay Pasachoff
The
following summary is based on evaluations by Dale Gary of our group at the JVLA
and Alphonse Sterling of NASA, a Hinode scientist:
What we did was looking at the
JVLA is to take radio images of an active region (AR), using the normally relatively-poor radio spatial resolution. We are then
using the Moon's limb as a knife edge; as the Moon
moves, we will look for sudden changes in the radio intensity, such as a sudden
drop-off over some frequency range. Via the timing we will know the
location on the AR of that feature to better than the normal radio spatial
resolution. By using Hinode and other opticla imaging spacecraft and ground-based telescopes, we
can see precisely what that feature was.
Another advantage in addition to
spatial resolution is that we also get better image quality because by
differencing the signal we get only signals from the narrow window covered by
the Moon. (At the frequencies we will be using, the dominant signal is from the
AR, rather than from the quiet-sun corona north and south of the AR along the
sliver that represents the differentiation.) The differencing removes the
confusion from the entire remainder of the disk.
At the frequencies we are using
(corresponding to wavelengths from 20 cm down to 6 mm), the resolution is
normally 6-12 arcsec. The limb of the Moon will move
about 0.5" per s, so if we have a stable enough signal we could get better
than a factor of 10 improvement in resolution.