Up: Imaging polarimetry of some clouds
For the purpose of calibration, we observed five different polarized and
one unpolarized standard stars taken from a list by Sekowski (1975). The
results
for the standard stars both "polarized'' and "unpolarized'' are reproduced
in Tables 2 and 3 respectively. For the standard polarized stars, the
observed polarization (p), error in polarization (
)
and position
angle (
)
are listed in Cols. 7, 8 and 9 of Table 2. The error in
position angle (PA) i.e.
though not listed in the table, can
be easily calculated by the relation (Serkowski 1974):
 |
(2) |
for
.
The Cols. 3, 4 and 5 represent the maximum polarization
value, corresponding position angle and wavelength as listed by
Serkowski (1975). A small discrepancy within the two sets of values can be due to
the fact that, Serkowski (1975) values are at a particular wavelength where
polarization becomes maximum. Whereas our
observations were carried out either in white light (W) or V filter
(
m). Since the interstellar polarization varies with
wavelength, what we should observe in the W filter
is an observed value of p which is somewhat lower than
.
Further,
if
also slightly varies with wavelength, the observed
will
be different from
.
However, this seems to be more unlikely
keeping in mind the constancy of
for interstellar polarization
(Coyne 1975).
At this stage without going into the details of wavelength dependence of
interstellar polarization, we conclude from Table 2. that,
the observed polarization values are matching with those enlisted by
Serkowski (1975) within errors. However, the PA (
)
values
show an average offset
of
for three nights in December 1997 and
for
April 01, 98.
The instrument was remounted on Apr. 02, 1998 due to technical reasons and
we observe a different
of
on April 02,
1998.
Now from our observations for the unpolarized standard star HD 114710
(in Table 3), we can conclude that our instrumental polarization is less
than 0.05%.
Up: Imaging polarimetry of some clouds
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