Published June 2, 2019 | Version v1
Conference paper Open

Phase-space spirals in Gaia DR 2: the role of the Milky Way bar

  • 1. Max Planck Institute for Extraterrestrial Physics, 85741 Garching, Germany, Institute of Astronomy, Russian Academy of Sciences, 48 Pyatnitskya St., Moscow 119017, Russia
  • 2. GEPI, Observatoire de Paris, PSL Universite, CNRS, 5 Place Jules Janssen, 92190 Meudon, France
  • 3. Max Planck Institute for Extraterrestrial Physics, 85741 Garching, Germany
  • 4. Observatoire de Paris, LERMA, CNRS, PSL Univ., UPMC, Sorbonne Univ., F-75014, Paris, France, College de France, 11 Place Marcelin Berthelot, 75005, Paris, France
  • 5. Astronomisches Rechen-Institut, Zentrum fur Astronomie der Universitat Heidelberg, Monchhofstr. 12-14, D-69120 Heidelberg, Germany, National Astronomical Observatories of China, Chinese Academy of Sciences, Datun Lu 20A, Chaoyang District, Beijing 100012, China, Main Astronomical Observatory, National Academy of Sciences of Ukraine, Akademika Zabolotnoho 27, 03680 Kyiv, Ukraine

Description

Using a single N-body simulation we explore the formation, evolution, and spatial variation of the phase-space spirals similar to those recently discovered in the Milky Way disk. For the first time in the literature we use a self-consistent N-body simulation of an isolated Milky Way-type galaxy to show that the phase-space spirals develop naturally from vertical waves driven by the buckling of the stellar bar.  Such vertical oscillations trigger the formation of various time-dependent phase-space spirals in the entire disk. The underlying physical mechanism implies the link between in-plane and vertical motion that leads  directly to phase-space structures whose amplitude and shape are in remarkable agreement with those of the phase-space spirals observed in the Milky Way disk. In our isolated galaxy simulation, phase-space spirals are still distinguishable  at the solar neighborhood 3 Gyr after the buckling phase.  The long-lived character of the phase-space spirals generated by the bar buckling instability cast doubts on the timing argument used so far to get back to the time of the onset of the perturbation.

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