** This is a special edition of CCD Views **
Table of Contents
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1. Monitor LS Peg for XMM Newton Observations
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1. MONITOR LS PEG FOR XMM NEWTON OBSERVATIONS
Dr. Darren Baskill (University of Leicester) has requested
optical observations of LS Peg (currently suspected as being
a DQ Her nova-like) to coincide with upcoming observations by the
XMM Newton X-Ray observatory.
Observations in are requested from now until July 8. Intensive,
time series observations are requested 12 hours before and
also during the actual XMM observation which is scheduled for June 6,
2005 from 08:55 - 21:34 (UT). So we need time series coverage from:
20:55 June 7 (UT) to 21:34 June 8 (UT)
Use an Ic filter if you have one and a V filter if not. Set your
exposure time for maximum precision. This is a bright system
(V~12) so it should be easy to get an SNR of 100. The latest ASAS-3
observation is:
May 13.4185 V=12.324 +/- 0.097
A new AAVSO f-scale chart has been prepared and is here:
http://www.aavso.org/cgi-bin/searchcharts3.pl?name=ls%20peg
Arne Henden has calibrated the field this week in BVRI so we
will be adding R and Ic magnitudes to the chart in a couple of
weeks.
Specifics science goals from Dr. Baskill:
"A possible 30.9 minute period was detected in the ASCA observation of LS
Peg, with an amplitude of 32%. Rodriguez-Gil et al (2001) independently
report a detection of a period at 29.6 min in the circular polarisation of
LS Peg. This coincidence suggests that the modulation in X-rays and
circular polarisation may have a common physical origin which warrants
further investigation.
XMM-Newton is currently scheduled to observe LS Peg for 10 hours on the
8th of June, 2005. Optically, LS Peg can usually be found around 12th
magnitude.
In looking deeper for a weaker period with XMM-Newton, we will validate
the method of identifying magnetic accretors from their spectra alone, a
method which works even at low signal-to-noise. This will establish X-ray
spectroscopy as a method for identifying & investigating magnetic
accreting systems. The extra signal-to-noise will also allow us to search
for periods in different energy bands, just like Patterson et al. (1998).
While XMM-Newton observes the heated gas at the white dwarf in X-rays,
and the inner disk at UV (with the XMM-Newton optical/UV monitor), we
would also like simultaneous high time resolution optical observations to
track the movement of gas from the outer disk. We would like this optical
data from 12 hours before the XMM-Newton observation, right through the
observation itself. In addition, in order to see more general changes in
the outer disk and what state the outer disk is in during the XMM-Newton
observation, we would like optical observations spanning several weeks
either side of the XMM-Newton observation."
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Good observing!
Aaron Price, AAVSO Technical Assistant (PAH)
Gary Walker, Chairman of the AAVSO CCD Committee (WGR)
Copyright 2005, American Association of Variable Star Observers
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THE AMERICAN ASSOCIATION OF VARIABLE STAR OBSERVERS
25 Birch Street, Cambridge, MA 02138 USA
Tel. 617-354-0484 Fax 617-354-0665
http://www.aavso.org
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