Spectropolarimetry of the Superwind Filaments of the Starburst Galaxy M 82: Kinematics of Dust Outflow

DOI DOI PDF 被引用文献9件 オープンアクセス
  • Michitoshi Yoshida
    1Hiroshima Astrophysical Science Center, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8526 yoshidam@hiroshima-u.ac.jp
  • Koji S. Kawabata
    1Hiroshima Astrophysical Science Center, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8526 yoshidam@hiroshima-u.ac.jp
  • Youichi Ohyama
    3Academia Sinica, Institute of Astronomy and Astrophysics, P.O. Box 23-141, Taipei 10617, Taiwan, R.O.C.

書誌事項

公開日
2011-03-25
権利情報
  • https://creativecommons.org/licenses/by-nc-nd/3.0/
DOI
  • 10.1093/pasj/63.sp2.s493
  • 10.48550/arxiv.1012.1503
公開者
Oxford University Press (OUP)

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説明

<jats:p>Spectropolarimetry results for the starburst galaxy M 82 are presented. The optical emission lines of the filaments in the energetic outflow (``superwind'') from the nuclear starburst region of M 82 are substantially polarized. The H$\alpha$ polarization degrees and angles measured by our study are consistent with previous narrowband imaging polarimetry data. The polarized emission lines are redshifted with respect to the emission lines in the total light and systemic motion of the galaxy. The emission line intensity ratios [N II]$/$H$\alpha$ and [S II]$/$H$\alpha$ in the polarized light are similar to those of the nuclear star-forming region. In addition, the electron density $N_{\rm e}$ derived from the [S II]$\lambda$6731$/\lambda$6717 line ratio of the polarized light is $\sim\ $600–1000 cm$^{-3}$ at a distance of more than 1 kpc from the nucleus, whereas the $N_{\rm e}$ derived from the total light are less than 300 cm$^{-3}$. These facts strongly suggest that the emission from the nuclear starburst of M 82 is scattered by dust grains entrained and transported outward by the superwind. A simple hollow biconical outflow model shows that the velocity of the outflowing dust grains, $v_{\rm d}$, ranges from 100 to 200 km s$^{-1}$ near the nucleus, decreases monotonically with the distance from the nucleus, and reaches $\sim\ $10 km s$^{-1}$ at around 1 kpc. The motion of the dust is substantially slower than that of both ionized gas ($v_{{\rm H}\alpha}$  $\sim\ $ 600 km s$^{-1}$) and molecular gas ($v_{\rm CO}$  $\sim\ $ 200 km s$^{-1}$) at the same distance from the nucleus of M 82. This indicates that dust grains in the superwind are kinematically decoupled from both gas components at large radii. Since the dust velocity $v_{\rm d}$ is much less than the escape velocity of M 82 ($v_{\rm esc}$  $\approx$ 170 km s$^{-1}$ at 1.5 kpc from the nucleus), most of the dust entrained by the superwind cannot escape to intergalactic space, and may fall back into the galaxy disk if there is no additional acceleration mechanism (such as radiation pressure).</jats:p>

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