Abstract:Most ultraluminous X-ray sources 1 (ULXs) display a typical set of properties not seen in Galactic stellar-mass black holes (BHs): higher luminosity (L x > 3 × 10 39 erg s −1 ), unusually soft X-ray components (kT 0.3 keV) and a characteristic downturn 2,3 in their spectra above ≈ 5 keV. Such puzzling properties have been interpreted either as evidence of intermediate-mass BHs 4,5 , or as emission from stellar-mass BHs accreting above their Eddington limit 6,7 , analogous to some Galactic BHs at peak luminosit… Show more
“…For instance, the recently reported 3.3 Hz and 5 Hz frequencies in the X-ray flux of M82 X-1 (Pasham, Strohmayer & Mushotzky 2014) could in fact turn out to be harmonics of 1.67 Hz, i.e., that source may be a P = 0.6 s pulsar. Another ULX, in NGC 7793, has an upper limit to the mass of the compact object of < 15M⊙, with allowed solutions in the neutron star mass range and phenomenology of state transitions similar to that of Her X-1 (Motch et al 2014).…”
If the ultraluminous source (ULX) M82 X-2 sustains its measured spin-up value oḟ ν = 10 −10 s −2 , it will become a millisecond pulsar in less than 10 5 yr. The observed (isotropic) luminosity of 10 40 erg/s also supports the notion that the neutron star will spin up to a millisecond period upon accreting about 0.1 M ⊙ -the reported hard X-ray luminosity of this ULX, together with the spin-up value, implies torques consistent with the accretion disc extending down to the vicinity of the stellar surface, as expected for low values of the stellar dipole magnetic field (B 10 9 G). This suggests a new channel of millisecond pulsar formation-in high-mass X-ray binaries (HMXBs)-and may have implications for studies of gravitational waves, and possibly for the formation of low-mass black holes through accretion-induced collapse.
“…For instance, the recently reported 3.3 Hz and 5 Hz frequencies in the X-ray flux of M82 X-1 (Pasham, Strohmayer & Mushotzky 2014) could in fact turn out to be harmonics of 1.67 Hz, i.e., that source may be a P = 0.6 s pulsar. Another ULX, in NGC 7793, has an upper limit to the mass of the compact object of < 15M⊙, with allowed solutions in the neutron star mass range and phenomenology of state transitions similar to that of Her X-1 (Motch et al 2014).…”
If the ultraluminous source (ULX) M82 X-2 sustains its measured spin-up value oḟ ν = 10 −10 s −2 , it will become a millisecond pulsar in less than 10 5 yr. The observed (isotropic) luminosity of 10 40 erg/s also supports the notion that the neutron star will spin up to a millisecond period upon accreting about 0.1 M ⊙ -the reported hard X-ray luminosity of this ULX, together with the spin-up value, implies torques consistent with the accretion disc extending down to the vicinity of the stellar surface, as expected for low values of the stellar dipole magnetic field (B 10 9 G). This suggests a new channel of millisecond pulsar formation-in high-mass X-ray binaries (HMXBs)-and may have implications for studies of gravitational waves, and possibly for the formation of low-mass black holes through accretion-induced collapse.
“…Outside the Local Group, NGC 300 X-1 ( »Ĺ 5 10 X 38 erg s −1 ; binary period »33 hr) shows X-ray dips, consistent with occultation from geometrically thick structures in the outer disk, or absorption in the wind of the donor star, but not with true eclipses (Binder et al 2015). A strong candidate for a true eclipse is the sharp dip in the Swift/X-ray Telescope flux recorded once from the ULX P13 in NGC 7793, at an orbital phase consistent with the inferior conjunction of its supergiant donor star (Motch et al 2014). However, there is no further confirmation of that single monitoring data point at subsequent epochs.…”
Section: Table 11mentioning
confidence: 99%
“…Modeling of the optical light curve from the irradiated donor star in NGC 7793-P13 showed (Motch et al 2014) that the source is viewed at an angle >20°and more likely much higher. Thus, in that case, super-Eddington accretion is the reason for the high luminosity, not a heavier BH or a down-the-funnel view.…”
We present the discovery, from archival Chandra and XMM-Newton data, of X-ray eclipses in two ultraluminous X-ray sources (ULXs), located in the same region of the galaxy M51: CXOM51 J132940.0+471237 (ULX-1, for simplicity) and CXOM51 J132939.5+471244 (ULX-2). Three eclipses were detected for ULX-1 and two for ULX-2. The presence of eclipses puts strong constraints on the viewing angle, suggesting that both ULXs are seen almost edge-on and are certainly not beamed toward us. Despite the similar viewing angles and luminosities ( »Ĺ 2 10 X 39 erg s −1 in the 0.3-8 keV band for both sources), their X-ray properties are different. ULX-1 has a soft spectrum, well fitted by Comptonization emission from a medium with electron temperature » kT 1 keV e . ULX-2 is harder, well fitted by a slim disk with » kT 1.5 in -1.8 keV and normalization consistent with a ∼10 M e black hole. ULX-1 has a significant contribution from multi-temperature thermal-plasma emission ( »Ĺ 2 10 X,mekal 38 erg s −1 ). About 10% of this emission remains visible during the eclipses, proving that the emitting gas comes from a region slightly more extended than the size of the donor star. From the sequence and duration of the Chandra observations in and out of eclipse, we constrain the binary period of ULX-1 to be either »6.3 days, or ≈12.5-13 days. If the donor star fills its Roche lobe (a plausible assumption for ULXs), both cases require an evolved donor, most likely a blue supergiant, given the young age of the stellar population in that Galactic environment.
“…Another class of objects thought to contain stellar-mass BHs are the ULX sources (Liu et al 2013, Motch et al 2014. Their X-ray luminosities (10 39 −10 41 erg s −1 ) exceed the Eddington limit for a NS by 1 − 3 orders of magnitude.…”
The relative phasing of the X-ray eclipse ephemeris and optical radial velocity (RV) curve for the X-ray binary IC10 X-1 suggests the He[λ4686] emission-line originates in a shadowed sector of the stellar wind that avoids ionization by X-rays from the compact object. The line attains maximum blueshift when the wind is directly toward us at mid X-ray eclipse, as is also seen in Cygnus X-3. If the RV curve is unrelated to stellar motion, evidence for a massive black hole evaporates because the mass function of the binary is unknown. The reported X-ray luminosity, spectrum, slow QPO, and broad eclipses caused by absorption/scattering in the WR wind are all consistent with either a low-stellar-mass BH or a NS. For a NS, the centre of mass lies inside the WR envelope whose motion is then far below the observed 370 km/s RV amplitude, while the velocity of the compact object is as high as 600 km/s. The resulting 0.4% doppler variation of X-ray spectral lines could be confirmed by missions in development. These arguments also apply to other putative BH binaries whose RV and eclipse curves are not yet phase-connected. Theories of BH formation and predicted rates of gravitational wave sources may need revision.
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