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Observation strategy for FOCAS polarimetry
Typical observation sequences
Linear spectropolarimetry
- Telescope rough pointing
- Fine pointing with Wollaston prism inserted
- Take a field image with mask (mask pattern image)
- Take a field image without mask (field image)
- Differential pointing
- Repeat steps (b) and (c) until pointing is correct
- Observation of target (repeat as required)
- with half-wave plate at PA= 0.0 deg
- with half-wave plate at PA=45.0 deg
- with half-wave plate at PA=22.5 deg
- with half-wave plate at PA=67.5 deg
- Observation of calibration sources
(if needed)
Linear imaging polarimetry
- Telescope rough pointing
- Fine pointing with Wollaston prism out
- Take a field image with mask (mask pattern image)
- Take a field image without mask (field image)
- Differential pointing
- Repeat steps (b) and (c) until pointing is correct
- Observation of target (repeat as required)
- with half-wave plate at PA= 0.0 deg
- with half-wave plate at PA=45.0 deg
- with half-wave plate at PA=22.5 deg
- with half-wave plate at PA=67.5 deg
- Observation of calibration sources
(if needed)
Circular spectropolarimetry
- Telescope rough pointing
- Fine pointing with Wollaston prism inserted
- Take a field image with mask (mask pattern image)
- Take a field image without mask (field image)
- Differential pointing
- Repeat steps (b) and (c) until pointing is correct
- Observation of target (repeat as required)
- with quarter-wave plate at PA= 45.0 deg
- with quarter-wave plate at PA=135.0 deg
- Observation of calibration sources (if needed)
Circular imaging polarimetry
- Telescope rough pointing
- Fine pointing with Wollaston prism out
- Take a field image with mask (mask pattern image)
- Take a field image without mask (field image)
- Differential pointing
- Repeat steps (b) and (c) until pointing is correct
- Observation of target (repeat as required)
- with quarter-wave plate at PA= 45.0 deg
- with quarter-wave plate at PA=135.0 deg
- Observation of calibration sources (if needed)
Exposure times
The estimation of total exposure time can be done in the same way as for normal
spectroscopy or imaging, except that polarimetry generally needs much
higher S/N. If the observer wants a polarimetric accuracy
dP = 0.1%, the error due to photon statistics should be nearly
equal to or less than 0.1%, i.e. the S/N should be nearly equal to or
higher than 1000. Resulting limiting magnitude of polarimetry is generally
5-7 mag brighter than the corresponding non-polarimetric observation
(i.e., normal spectroscopy or imaging).
Since the incident light is devided into two beams in FOCAS polarimetry,
the saturation-free exposure time per an image becomes roughly twice as
long as that of non-polarimetric observation.
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