2012
DOI: 10.1134/s1990341312040074
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Technique of polarimetric observations of faint objects at the 6-m BTA telescope

Abstract: We describe the technique of spectropolarimetric observations allowing for the measurements of the Stokes parameters in one of the observational modes of the SCORPIO focal reducer of the 6-m BTA telescope of the SAO RAS. The characteristics of the instrument in the spectropolarimetric mode of observations are given. We present the algorithm of observational data reduction. The capabilities of the SCORPIO spectropolarimetric mode are demonstrated on the examples of observations of various astronomical objects.

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Cited by 69 publications
(59 citation statements)
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“…Additionally, we observed non-polarized stars as spectrophotometric standards. We found that the accuracy of the linear polarization measurements is ∼ 0.1% (more details in Afanasiev & Moiseev 2005;Afanasiev & Amirkhanyan 2012;Afanasiev et al 2014a). The typical differences between our measurements of polarization standards and these in the catalogue were 0.1-0.2% for polarization and 2-4 degrees for the polarization angle.…”
Section: Observationmentioning
confidence: 81%
“…Additionally, we observed non-polarized stars as spectrophotometric standards. We found that the accuracy of the linear polarization measurements is ∼ 0.1% (more details in Afanasiev & Moiseev 2005;Afanasiev & Amirkhanyan 2012;Afanasiev et al 2014a). The typical differences between our measurements of polarization standards and these in the catalogue were 0.1-0.2% for polarization and 2-4 degrees for the polarization angle.…”
Section: Observationmentioning
confidence: 81%
“…In each epoch a series of the images was shot to take into account the variation of the atmosphere. The method of polarimetric observations with SCORPIO is described in Afanasiev & Amirkhanyan (2012). We obtained Mrk 6 spectra from 12 epochs in the 2010-2013 monitoring period.…”
Section: Observational Testmentioning
confidence: 99%
“…In this polarimetric mode of the instrument, an achromatic half-wave phase plate and a Wollaston prism are installed before a prism. The Wollaston prism, separating the beam into the ordinary o and extraordinary e rays by 5 deg (2 on the celestial sphere), is inserted in the parallel beam (Afanasiev et al, 2012). We use the mask (high 2 and diameter 4), which cuts non-overlapping area.…”
Section: Single Wollaston Prismmentioning
confidence: 99%