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X-ray binaries with ALMA in Q-band. Tom Maccarone (University of Southampton) . Classes of sources. Black hole X-ray binaries Neutron star X-ray binaries Focus on low B neutron stars High B disrupts accretion disk and no jets are seen White dwarf binaries
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X-ray binaries with ALMA in Q-band • Tom Maccarone (University of Southampton)
Classes of sources • Black hole X-ray binaries • Neutron star X-ray binaries • Focus on low B neutron stars • High B disrupts accretion disk and no jets are seen • White dwarf binaries • Focus here will be on black hole X-ray binaries Computer generated image of GRO J1655-40, made using Rob Hynes' visualization tool
ING archive/Nick Szymanek Russell et al. 2007 Stirling et al. 2001
The fundamental advantages of X-ray binaries over AGN for understanding black hole jets • Viscous timescale from inner disk in typical AGN is ~decades • Less than this from the outer edge of the disk in most XRBs • Many XRBs vary by 7 orders of magnitude in luminosity on years timescales • Allows flux-flux correlations to be useful • Sources are brighter than AGN in most wavebands, allowing high S/N detections • Comparing AGN with XRBs gives a much bigger lever arm on mass effects than AGN alone • Masses are also better measured • BHXRBs are close in mass to neutron stars, allowing for testing whether the BH itself is important or just the deep potential well
Jet-disk coupling in the low/hard state • LR LX0.7 • In agreement with relatively simple models for jet production provided LX mdot2 • This L-mdot relation comes from ADAF models • Faint sources are flat spectrum, so frequency of observations doesn't matter • But also means higher frequency is closest to the black hole • Not clear why the high luminosity intermediate states lie on the extrapolation of this relation. • X-ray spectra and hence geometry is quite different • Radio emission for many data points in that region are for optically thin emission from Gallo, Fender & Pooley (2003)
Neutron star jets • Fainter than black holes when hard X-rays are strong • consistent with square of black hole relation, implying advection in black holes, but surface effects in neutron stars (Koerding et al. 2006) • But still based on small number of points with relatively large uncertainties • Better sensitivity is essential for such faint objects • Brighter than black holes in soft states • not yet well understood, but maybe a boundary layer effect (e.g. Livio 1999; Maccarone 2009)? from Migliari & Fender 2006
Rapid variability From Hynes et al. 2009 From Gallo et al. 2006
Some open questions • What happens at very low radio luminosity? • Is there soft state emission from black hole X-ray binaries? • There is scatter in the L_X vs L_R relation. How much is due to: • Real physical scatter that requires complex explanations? • BH spin? • Variable relationships of magnetic field to equipartition (e.g. Pe'er & Casella 2009) • Non-simultaneity of data (i.e. rapid variability)? • Highest frequencies best for studying rapid variability • Would like to monitor over hours to days timescales in radio and X-rays
Quiescent black hole X-ray binaries • Important for understanding physics of accretion • Also useful for understanding black hole populations • Most black hole X-ray binaries spend most of their time in quiescence (i.e. LX ~ 1031-32 ergs/sec) • Surveys of the Galactic Plane/GC region in radio combined with other wavelengths should allow a real population study of quiescent black hole X-ray binaries • Should be ~1000-10000 BH XRBs in the Galaxy (e.g. Romani 1992; Portegies Zwart et al. 1997) • A survey for quiescent black hole X-ray binaries should produce a large enough sample to say something real about the mass distribution of black holes in binaries
Globular cluster black holes in the Galaxy 47 Tuc – X-ray from Heinke et al., FUV from Knigge et al. • Recent extragalactic globular cluster work shows good evidence for stellar mass black holes • None known in Milky Way clusters • BUT quiescent cataclysmic variables and qBHXBs look almost identical in optical/UV/X-rays • Radio emission at 5-10 Jy should be detectable from qBHXBs, but not from qDNe
Neutron star X-ray binaries • Is LR really prop. to Lx1.4? • Any correlation with rotation rate? • Do all neutron stars show soft state radio emission? • What causes this emission? • What are the spectral shapes for emission from low L neutron star accretors? • Does the BH analogy hold up for spectra? • Also, maybe worth another look at the high B neutron stars Migliari & Fender 2006
ALMA vs EVLA • Southern hemisphere a key advantage • Most X-ray binaries are in/near the Galactic Plane • Also opens up the LMC sources, which have known distances, a key problem for most current X-ray binary studies • Plus, the opportunity to go up to higher frequencies
ALMA vs ATCA • Big advantage for rapidly variable sources if multi-wavelength spectral energy distributions wanted • ALMA at the same longitude as the VLT, VLA • In some cases will allow nearly uninterrupted frequency coverage from 1 GHz to 10^21 Hz, with data taken nearly simultaneously • Not possible from Australia, especially for optically faint sources
Why Q-band? • Transient phenomena • Black hole X-ray binary outbursts typically happen 1-2 times per year • Don't want to be limited by weather during these outbursts • Larger field of view for cases of new X-ray transients, star clusters • Want some frequency overlap with the Compact Array • Will allow 24-hour coverage during outbursts
Conclusions • X-ray binaries probe interesting ranges of parameter space for jet physics • They are highly, rapidly variable phenomena. Flexible scheduling needed, and continuous coverage for days could produce interesting results • High frequency variability likely to be the fastest variability – high sensitivity, high frequency observations most likely to see the most interesting things • ALMA is in the best hemisphere for observing these sources, both in terms of latitude and longitude