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Nature of X-ray transients in the Magellanic Clouds : (Be/X-ray pulsars, and Supersoft sources) Andry RAJOELIMANANA 1, 2 ‏ Supervisor : Prof Phil CHARLES.

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Presentation on theme: "Nature of X-ray transients in the Magellanic Clouds : (Be/X-ray pulsars, and Supersoft sources) Andry RAJOELIMANANA 1, 2 ‏ Supervisor : Prof Phil CHARLES."— Presentation transcript:

1 Nature of X-ray transients in the Magellanic Clouds : (Be/X-ray pulsars, and Supersoft sources) Andry RAJOELIMANANA 1, 2 ‏ Supervisor : Prof Phil CHARLES 3 Co-supervisor : Prof Brian Warner 1 1 University of Cape Town (UCT), 2 South African Astronomical Observatory (SAAO) 3 School of Physics and Astronomy, Southampton University

2 Outline  Be/X-ray transients  Introduction  Long-term properties  SALT/RSS spectroscopy.  Supesoft sources : CAL83 and RX J0513-6935  Long-term properties  Orbital periodicities.  X-ray spectroscopy.  X-ray/optical anti-correlation.  Summary

3 Be/X-ray pulsar (BeX) Be Star + X-ray pulsar Transient X-ray sources (Lx~10 37 erg.s -1 ) Wide and eccentric orbit (0.1<e<0.9) Accretion from the Be equatorial disc

4 Long-term variations (18 yrs observation) (Rajoelimanana, Charles & Udalski., 2011,MNRAS, 413,1600) MACHO and OGLE light curves

5 V vs. V-R diagram Loop-like structure. “Be – Normal B – Be” star transitions. Disk-less phase Disk formation Disk dissipation SXP18.3

6 Optical high state Optical low state SALT/RSS Broad-band Spectra Normal B-star Be star

7 SALT/RSS High resolution Blue Spectra Spectral classification (temperature criteria). Rotational velocities.

8 Outbursts amplitude vs. brightness The strength of the outburst increases with the brightness of the source.

9 Evolution of the line profiles in A0538-66 Outburst Before After phase=1.0 phase=1.24 phase=0.87 Disk-less phase

10 Orbital and super-orbital period correlation Rajoelimanana, Charles & Udalski., 2011,MNRAS, 413,1600 Shorter period : truncated at smaller radius

11 Supersoft X-ray sources (SSS)

12 Supersoft X-ray sources (SSS)‏ T BB ~ 20-50 eV L bol ~ 10 37 - 10 38 erg s -1 Supersoft emission < 0.5 keV SSS system :  WD + Sub-giant companion  High accretion rate > 10 -7 M sun yrs -1 WD burns H steadily at its surface Orbital period : P orb < ~1 d

13 Long-term MACHO and OGLE light curves CAL 83 Timescale ~ 450 d Optical minima duration : ~ 200 d RXJ 0513.9-6951 Timescale ~ 170 d Optical minima duration : ~ 30 d (Rajoelimanana, et al 2011 (in prep))

14 Orbital periodicity Detrend: subtract a linear fit. Refinement of the orbital periods using 18 yrs light curves CAL 83 P orb = 1.04752 +/- 0.00001 RX J0513.9-6951 P orb = 0.76295 +/- 0.00001 d Rajoelimanana, Charles & Udalski., 2011 (in prep)

15  EPIC-PN spectra fitted by blackbody model (using Xspec)  nH=6.5 x 10 20 cm -3 (frozen, HST) XMM-Newton spectra of CAL83 (Rajoelimanana, et al 2011 (in prep))

16 X-ray / Optical anti-correlation in CAL83 Optical low X-ray on Optical high X-ray off or very weak T bb from 40 keV to 25 keV (Rajoelimanana, et al 2011 (in prep))

17 X-ray / Optical anti-correlation Optical low X-ray on Optical high X-ray off or very weak Contraction model : (Southwell et al., 1996)‏  Accretion rate drops R wd decreases (Optical brightness decreases)  rise in effective temperature (from ~ 25 keV to 40 keV)  increase in X-ray luminosity No X-ray emissions detected during optical high state peak of the emission is SHIFTED from the supersoft X-ray to the UV

18 Summary  Be/X-ray transients  Loop-like structure in the colour magnitude diagram.  Disk-less, disk formation, disk dissipation phases.  Broad-band spectra : “Be – Normal B – Be star” transitions.  High resolution spectra : Spectral classifications and rotational velocities.  Correlation between orbital and super-orbital periodicities  Supesoft sources : CAL83 and RX J0513-6935  Long-term variations on timescales of 450 d and 170 d, respectively  Refinement of their orbital periodicities.  Anti-correlation between X-ray count rate and optical brightness.  Anti-correlation between blackbody temperatures/luminosities and optical brightness (Contraction model).  The peak of the emission is shifted from supersoft X-ray into the UV during optical high state.

19 Thank you


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