NICMOS Polarimetry Update
Note that the coefficients presented below supersede all previous values!
Dean C. Hines
NICMOS Project
Steward Observatory
The University of Arizona
Tucson, AZ 85721
dhines@as.arizona.edu
NICMOS contains optics which enable imaging polarimetry at 1 &
2 microns with unprecedented detail. The preflight Thermal Vacuum tests revealed
that each polarizer has a unique polarizing efficiency, and that the position angle
offsets differ from the nominal positions of 0, 120 & 240. Therefore, to properly
reduce polarimetry data obtained with NICMOS, a new algorithm different from that
needed for an ideal polarizer was developed. Combined with calibration measurements
of polarized and unpolarized stars, this algorithm allows accurate imaging polarimetry
to about +/- 0.5% (in percentage polarization) over the entire field of view in both
cameras.
The HSL Algorithm for Reducing NICMOS Polarimetry
Observations
The ``standard theory'' polarimetry reduction algorithm outlined
in the original NICMOS Manual assumes that the polarizers have uniform and perfect
(100%) polarizing efficiencies, and that the position angles of the primary axis
of the polarizers are offset by exactly 120. The thermal vacuum tests showed that
the NICMOS polarizers are not ideal, so a more complex technique is required. The
new algorithm developed by Hines, Schmidt & Lytle (1997; hereafter HSL) is presented
below.

The characteristics of the polarizers and the coefficients for
the HSL algorithm are presented below. These were determined during Preflight Thermal
Vacuum tests and from on-orbit measurements of polarized and unpolarized stars.
Note that the coefficients presented
herein supersede all previous values!
Table 1: Characteristics of the NICMOS Polarizers
|
| Filter |
phi_k
|
epsilon_k
|
t_k
|
l_k
|
Comments
|
| POL0S |
1.42
|
0.9717
|
0.7760
|
0.0144
|
``ghost'' images
|
| POL120S |
116.30
|
0.4771
|
0.5946
|
0.3540
|
|
| POL240S |
258.72
|
0.7682
|
0.7169
|
0.1311
|
``ghost'' images
|
|
| POL0L |
8.84
|
0.7313
|
0.8981
|
0.1552
|
...
|
| POL120L |
131.42
|
0.6288
|
0.8551
|
0.2279
|
...
|
| POL240L |
248.18
|
0.8738
|
0.9667
|
0.0673
|
...
|
|
Note: Ghost images are definitely present
in POL0S and POL240S in exposures of very bright targets. No such ghosting is apparent
in the NIC2 polarizers.

These ghosts will typically be seen as regions of 100%
polarization (seen as white blobs in the lower right panel), since they appear in
different positions in the POL0S and POL240S. There are no obvious ghosts in POL120S.
Note that the object was very bright with J=7.32
Table 2: Coefficients for Simultaneous Solution
| Filter |
A_k
|
(epsilon_k)*B_k
|
(epsilon_k)*C_k
|
| POL0S |
+0.3936
|
+0.3820
|
+0.0189
|
| POL120S |
+0.4025
|
-0.1166
|
-0.1526
|
| POL240S |
+0.4054
|
-0.2876
|
+0.1195
|
|
| POL0L |
+0.5187
|
+0.3614
|
+0.1152
|
| POL120L |
+0.5250
|
-0.0411
|
-0.3276
|
| POL240L |
+0.5159
|
-0.3262
|
+0.3111
|
|
References:
Hines, D.C., 1998: Imaging Polarimetry with NICMOS (Entire Report in PostScript)
[Contains updated coefficients as listed above].
Hines, D.C., Schmidt, G.D., & Lytle, D. 1997, The Polarimetric Capabilities of
NICMOS, in The 1997
HST Calibration Workshop with a New Generation of Instruments, ed. Casertano
et al. (Contains old coefficients)
NICMOS Instrument
Manual (Contains standard theory algorithm)
|
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