SS433's Jet Trace from ALMA Imaging and Global Jet Watch Spectroscopy: Evidence for Post-launch Particle Acceleration

We present a comparison of Doppler-shifted Hα line emission observed by the Global Jet Watch from freshly launched jet ejecta at the nucleus of the Galactic microquasar SS433 with subsequent Atacama Large Millimeter/submillimeter Array (ALMA) imaging at mm-wavelengths of the same jet ejecta. There is a remarkable similarity between the transversely resolved synchrotron emission and the prediction of the jet trace from optical spectroscopy: this is an a priori prediction and not an a posteriori fit, confirming the ballistic nature of the jet propagation. The mm-wavelength of the ALMA polarimetry is sufficiently short that the Faraday rotation is negligible and therefore that the observed -vector directions are accurately orthogonal to the projected local magnetic field. Close to the nucleus, the -field vectors are perpendicular to the direction of propagation. Further out from the nucleus, the -field vectors that are coincident with the jet instead become parallel to the ridge line; this occurs at a distance where the jet bolides are expected to expand into one another. X-ray variability has also been observed at this location; this has a natural explanation if shocks from the expanding and colliding bolides cause particle acceleration. In regions distinctly separate from the jet ridge line, the fractional polarization approaches the theoretical maximum for synchrotron emission.

[1]  K. Blundell,et al.  Fast launch speeds in radio flares, from a new determination of the intrinsic motions of SS 433's jet bolides , 2016, 1606.01240.

[2]  R. Paladino,et al.  ALMA SCIENCE VERIFICATION DATA: MILLIMETER CONTINUUM POLARIMETRY OF THE BRIGHT RADIO QUASAR 3C 286 , 2016, 1605.00051.

[3]  Baltasar Vila-Vilaro,et al.  The human pipeline: distributed data reduction for ALMA , 2014, Astronomical Telescopes and Instrumentation.

[4]  T. Cornwell,et al.  A multi-scale multi-frequency deconvolution algorithm for synthesis imaging in radio interferometry , 2011, 1106.2745.

[5]  K. Blundell,et al.  SS433's accretion disc, wind and jets: before, during and after a major flare , 2011, 1104.2917.

[6]  S. Migliari,et al.  Coupled Radio and X-Ray Emission and Evidence for Discrete Ejecta in the Jets of SS 433 , 2008, 0804.1337.

[7]  D. H. Roberts,et al.  Structure and Magnetic Fields in the Precessing Jet System SS 433. I. Multifrequency Imaging from 1998 , 2007, 0712.2005.

[8]  K. Blundell,et al.  The Distance to SS433/W50 and its Interaction with the ISM , 2007, 0707.0506.

[9]  K. Blundell,et al.  Jet Velocity in SS 433: Its Anticorrelation with Precession-Cone Angle and Dependence on Orbital Phase , 2004, astro-ph/0410457.

[10]  A. M. Stirling,et al.  Polarization and kinematic studies of SS 433 indicate a continuous and decelerating jet. , 2004 .

[11]  K. Blundell,et al.  Symmetry in the Changing Jets of SS 433 and Its True Distance from Us , 2004, astro-ph/0410456.

[12]  K. Blundell,et al.  Rapid variability of the arcsec-scale X-ray jets of SS 433 , 2004, astro-ph/0501097.

[13]  A. M. Stirling,et al.  Radio‐emitting component kinematics in SS433 , 2002 .

[14]  S. Migliari,et al.  Iron Emission Lines from Extended X-ray Jets in SS 433: Reheating of Atomic Nuclei , 2002, Science.

[15]  P. B. Cameron,et al.  Twenty Years of Timing SS 433 , 2001, astro-ph/0107296.

[16]  K. Johnston,et al.  Radio emission from conical jets associated with X-ray binaries , 1988 .

[17]  Bruce Margon,et al.  Observations of SS 433 , 1984 .

[18]  K. Johnston,et al.  An analysis of the proper motions of SS 433 radio jets , 1981 .