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This paper discusses the monitoring and analysis of state transitions in the supersoft source CAL 83 using XMM observations. It explores the variability patterns and spectral changes in the X-ray and optical domains, providing insights into the source's physical properties and accretion processes.
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XMM monitoring of the state transition of the supersoft source CAL 83 Robert Schwarz Astrophysikalisches Institut Potsdam Jochen Greiner MPE Garching Gloria Sala Uni Barcelona Ronald Mennickent Uni Concepcion Super Soft X-ray Sources – New developments ESAC, May 18, 2009
Canonical SSS source in the LMC 1-day orbital period Low amplitude orbital modulation in optical and X-rays Inclination < 30 Tentative X-ray pulsations at 38 min Introducing CAL 83
Good fit to the data with a NLTE model (Lanz et al. 2004) log g = 8.5, Teff = 500 kK Suggests a massive WD of 1.3 Msun High-resolution X-ray spectrum
MACHO light curve (Greiner & di Stefano 2002) X-ray off-states in CAL 83
ObservationsofRXJ 0513-69 Short transition times only high or low states X-ray on state shorter than off state Anti-correlated brightness changes in SSS
Anti-correlated brightness changes in SSS Models • Expansion and cooling of the envelope • Limit cycle regulated by changing mass accretion rate Reinsch et al. 2000 • Radius/temperature changes of the WD • Increased irradiation of the outer disk Hachisu & Kato 2003 • Stripping of the companions surface by a strong wind • X-ray off: wind absorption optical high: expanded disk
Similar pattern Different timescale Comparison with MACHO observations
Recurrence time: 430 days Duty cycle: 50% Long term behaviour from OGLE
Sharp drop (t < 1 d) to intermediate brightness level Immediate recovery (t ~ 20 d) X-ray detection during optical high state Anti-correlation of optical and X-ray over a wide range X-ray/optical lightcurves
Low resolution X-ray spectroscopy Blackbody fits Correlation between Nh and kTbb
Black: April 2000 (Lanz et al. 2004) Red: August 2008 High state RGS spectrum
Free fits: kTbb varies from 25 to 33 eV fixing Nh to 8 x 1020 cm-2 kTbb varies from 23 to 37 eV Luminosity increases and radius shrinks changes by factor of 2 Spectral variation
Changes of the X-ray spectra can not explain the UV variation.. Broadband spectral energy distribution
Fix temperature and luminosity to the value of the high state spectrum Cold absorption fails Ionized absorber Nh= 4 1022 cm-2 X-ray variation by strong absorption only?
New complex variability patterns 1. short repetition time 2. Long transitions to optical high state Long term variability Ambiguous X-ray spectroscopy 50% temperature change or strong ionized absorber Tight anti-correlation between optical and X-rays Summary