IGR J19552+0044: A new asynchronous short period polar: "Filling the gap between intermediate and ordinary polars"
G. Tovmassian, D. Gonzalez-Buitrago, J. Thorstensen, E. Kotze, H., Breytenbach, A. Schwope, F. Bernardini, S. V. Zharikov, M. S. Hernandez, D., A. H. Buckley, E. de Miguel, F.-J. Hambsch, G. Myers, W. Goff, D. Cejudo, D., Starkey, T. Campbell, J. Ulowetz, W. Stein, P. Nelson

TL;DR
This paper confirms IGR J19552+0044 as an asynchronous polar with the largest known asynchronism, achieved through detailed optical and X-ray observations revealing its complex variability and magnetic properties.
Contribution
It provides the first definitive classification of IGR J19552+0044 as an asynchronous polar with a significant asynchronism degree, filling the gap between intermediate and ordinary polars.
Findings
Confirmed IGR J19552+0044 as an asynchronous polar
Discovered the largest known asynchronism degree in polars
Identified cyclotron emission indicating a magnetic field below 20 MG
Abstract
Based on XMM--Newton X-ray observations IGR J19552+0044 appears to be either a pre-polar or an asynchronous polar. We conducted follow-up optical observations to identify the sources and periods of variability precisely and to classify this X-ray source correctly. Extensive multicolor photometric and medium- to high-resolution spectroscopy observations were performed and period search codes were applied to sort out the complex variability of the object. We found firm evidence of discording spectroscopic (81.29+/-0.01m) and photometric (83.599+/-0.002m) periods that we ascribe to the white dwarf (WD)\ spin period and binary orbital period, respectively. This confirms that IGR J19552+0044 is an asynchronous polar. Wavelength-dependent variability and its continuously changing shape point at a cyclotron emission from a magnetic WD with a relatively low magnetic field below 20 MG. The…
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Taxonomy
TopicsAstrophysical Phenomena and Observations · Stellar, planetary, and galactic studies · Pulsars and Gravitational Waves Research
