OMC-INTEGRAL: OPTICAL OBSERVATIONS OF X-RAY BINARIES M.D. Caballero-García1, A. Domingo1, D. Rísquez1, J.M. Mas-Hesse2, A. Jiménez3, F. Figueras4,5, C. Jordi4,5 1LAEFF-INTA Madrid (Spain (Spain)) 2CAB-INTA Madrid (Spain (Spain)) 3ESTEC-ESA Noordwijk (The (The Netherlands) Netherlands) 4UB Barcelona (Spain (Spain)) 5IEEC Barcelona (Spain (Spain)) JENAM 2004, Granada Summary Ø Cyg X-1: temporal analysis (simultaneous optical, high and low energy light curves). Ø ROSAT sources probably detected in the optical band by OMC. Ø LMC X-4: optical light curve. Cyg X-1 Ø Ø Ø Ø HMXB discovered in 1962. The optical counterpart (HD 226868/V1357 Cyg) discovered by Bolton 1972 and Webster & Murdin 1972. Masses: 17.5 Msun for the optical counterpart (O9.7Iab) and 10.1 Msun for the black hole (Herrero et al. 1995). The blue giant is filling the Roche Lobe and is transferring mass into the black hole. Optical light curve period: 5.599836±0.000024 days (Brocksopp et al. 1999). This corresponds to the orbital period of the system. Distance: 1700 pc Cyg X-1 Optical light curve Ø Double-peaked ellipsoidal modulation due to the tidally and rotationally distorted star. <Amplitude>=0.06 mag. τ = 5.6 days Inclination of the orbit: i ≈ 40-60º (Bruevich et al. 1978) Ø Cyg X-1 Correlation with X-rays INTEGRALà simultaneous measurements of the same field in optical (OMC) and hard Xrays (IBIS). Rev. 16-18. Ø X-ray flares in the scale of a few days probably due to focalization of the supergiant’s wind by the BH. Ø The X-ray flares correspond to optical minima. à optical-x-ray correlations will be studied in the future. Ø OMC data (top panel) and IBIS-ISGRI (bottom panel, courtesy of A. Bazzano and the ISGRI team). Cyg X-1 SPI: γ-ray spectrograph Multiwavelength correlation IBIS: γ-ray imager Ø Ø Ø Simultaneous measurements of the same field in optical (OMC), hard X-rays (SPI and IBIS) and soft X-rays (JEMX). Rev. 79-80. Once more the highest high energy flares corresponds to optical minima. INTEGRAL Þ flares are real. OMC Þ relation with the orbital configuration. JEM-X: X-rays radio OMC: optical SPI, IBIS, JEM-X radio and OMC data (top to bottom). ROSAT sources Ø Ø Ø OMC monitors ∼ 100 stars in each field, all extracted from The OMC Input Catalogue (Domingo et al. 2003). ROSAT catalogues (Bright and Faint) are included. OMC extracts the photometric information from the photon counting of pixels in a 11x11 pixels box centered on the ROSAT coordinates. 5 ROSAT sources monitored (distance to ROSAT coordinates < 30 arcsec, inside the ROSAT error circle) showed a large degree of variability in the optical band, unknown before. à Possible optical counterparts of the ROSAT sources. OMC 3’x3’ photometric box ROSAT sources Optical light curves Ø Names of the sources: IOMC 0237000035 ↔ 1RXS J095156.0+004722 IOMC 1306000026 ↔ 1RXS J054101.8+203624 IOMC 2674000067 ↔ 1RXS J200219.0+333912 IOMC 2675000078 ↔ 1RXS J200912.0+323344 IOMC 4896000046 ↔ 1RXS J095706.3-012019 Ø Ø Ø Ø Optical variations typical of binary systems (blue fig.). Periods ranging from 0.4 to 1.9 days. Spectral types ranging from F to K. V magnitudes relatively bright (from 8.9 to 11.5). Observations in X-rays will be made in the future. IOMC 2675000078 IOMC 0237000035 IOMC 4896000046 IOMC 1306000026 IOMC 2674000067 ROSAT sources Ø Binary system of contact type. Ø τ = 0.42233 ± 0.00003 days Ø G0 spectral type. Ø 14’’ away from 1RXS J200912.0+323344 IOMC 2675000078 ROSAT sources Ø Binary system of contact type. Ø τ = 0.46515 ± 0.00018 days Ø F8 spectral type. Ø 8’’ away from 1RXS J095156.0+004722 IOMC 0237000035 ROSAT sources Ø Binary system of detached type. Ø τ = 0.9871 ± 0.0008 days Ø F5 spectral type. Ø 20’’ away from 1RXS J095706.3-012019 IOMC 4896000046 ROSAT sources Ø Probably pulsating stars. Ø Light curves not folded with the period. Ø K2 and G8 spectral types. Ø 8’’ away from 1RXS J054101.8+203624 and 41.7’’ away from 1RXS J200219.0+333912 IOMC 1306000026 IOMC 2674000067 LMC X-4 Ø Ø Ø Ø It is a HMXB with a possible neutron star as the compact object. Ellipsoidal modulation in the optical light curve due to the tidally and rotationally distorted star. ∆V = 0.4 mag. τ = 1.4 days Faint (V∼14) and located in an optically crowded field (LMC). The OMC extracted photometric box (∼1’) is strongly affected by the nearby stars. LMC X-4 OMC 3’x3’ photometric box Optical light curve Ø Ø Ø Some dispersion is intrinsic to the source. A sinusoidal fit to the light curve was made to know the parameters τ and ∆V. Values obtained: ∆Vcalculated=0.036 mag. τcalculated=1.35 days in agreement with that we expected. OMC data fitted with a sinus function.
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