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Fermi bubble simulations: black hole feedback in the Milky Way

Published online by Cambridge University Press:  22 May 2014

M. Ruszkowski
Affiliation:
Department of Astronomy, University of Michigan, Ann Arbor, MI, USA email: [email protected], [email protected]
H.-Y. K. Yang
Affiliation:
Department of Astronomy, University of Michigan, Ann Arbor, MI, USA email: [email protected], [email protected]
E. Zweibel
Affiliation:
Department of Astronomy and Physics, University of Wisconsin Madison, Madison, WI, USA email: [email protected]
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Abstract

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The Fermi γ-ray telescope discovered a pair of bubbles at the Galactic center. These structures are spatially-correlated with the microwave emission detected by the WMAP and Planck satellites. These bubbles were likely inflated by a jet launched from the vicinity of a supermassive black hole in the Galactic center. Using MHD simulations, which self-consistently include interactions between cosmic rays and magnetic fields, we build models of the supersonic jet propagation, cosmic ray transport, and the magnetic field amplification within the Fermi bubbles. Our key findings are that: (1) the synthetic Fermi γ-ray and WMAP microwave spectra based on our simulations are consistent with the observations, suggesting that a single population of cosmic ray leptons may simultaneously explain the emission across a range of photon energies; (2) the model fits the observed centrally-peaked microwave emission if a second, more recent, pair of jets embedded in the Fermi bubbles is included in the model. This is consistent with the observationally-based suggestion made by Su & Finkbeiner (2012); (3) the radio emission from the bubbles is expected to be strongly polarized due to the relatively high level of field ordering caused by elongated turbulent vortices. This effect is caused by the interaction of the shocks driven by the jets with the preexisting interstellar medium turbulence; (4) a layer of enhanced rotation measure in the shock-compressed region could exist in the bubble vicinity but the level of this enhancement depends on the details of the magnetic topology.

Type
Contributed Papers
Copyright
Copyright © International Astronomical Union 2014 

References

Carretti, E., Crocker, R. M., Staveley-Smith, L., et al. 2013, Nature 493, 66Google Scholar
Crocker, R. M. & Aharonian, F. 2011, Phys. Rev. Lett. 106, 101102CrossRefGoogle Scholar
Finkbeiner, D. P. 2004, ApJ 614, 186Google Scholar
Larsson, J. & Lele, S. K. 2009, Physics of Fluids 21, 126101Google Scholar
Li, Z., Morris, M. R., & Baganoff, F. K. 2013, arXiv: 1310.0146Google Scholar
Planck Collaboration 2013, A&A 554, A139Google Scholar
Su, M., Slatyer, T. R., & Finkbeiner, D. P. 2010, ApJ 724, 1044Google Scholar
Su, M. & Finkbeiner, D. P. 2012, ApJ 753, 61Google Scholar
Strong, A. W., et al. 2007, Annual Review of Nuclear and Particle Science 57, 285Google Scholar
Yang, H.-Y. K., Ruszkowski, M., & Zweibel, E. 2013, MNRAS 2432, arXiv:1307.3551Google Scholar
Yang, H.-Y. K., Ruszkowski, M., Ricker, P. M., Zweibel, E., & Lee, D. 2012, ApJ 761, 185Google Scholar