Superwind-Driven Intense H2 Emission in NGC 6240
Youichi Ohyama, Michitoshi Yoshida, Tadafumi Takata, Masatoshi Imanishi, Tomonori Usuda, Yoshihiko Saito, Hiroko Taguchi, Noboru Ebizuka, Fumihide Iwamuro, Kentaro Motohara, Tomoyuki Taguchi, Takashi Hata, Toshinori Maihara, Masanori Iye, Toshiyuki Sasaki, George Kosugi, Ryusuke Ogasawara, Junichi Noumaru, Yoshihiko Mizumoto, Masafumi Yagi, Yoshihiro Chikada
Abstract
We have performed a long-slit K band spectroscopic observation of the luminous infrared galaxy NGC 6240. The peak position of the H2 v=1-0 S(1) emission in the slit is located ~0.3" - 0.4" north of the southern nucleus. It is almost the midpoint between the southern nucleus and the peak position of the 12CO J=1-0 emission. Based on the line-ratio analyses, we suggest the excitation mechanism of H2 is pure thermal at most positions. In the southern region we find the following three velocity components in the H2 emission: the blueshifted shell component (~-250 km s-1 with respect to Vsys) which is recognized as a distinct C-shape distortion in the velocity field around the southern nucleus, the high-velocity blueshifted ``wing'' component (~-1000 km s-1 with respect to Vsys), and the component indicating possible line splitting of ~500 km s-1. The latter two components are extended to the south from the southern nucleus. We show that the kinematic properties of these three components can be reproduced by expanding motion of a shell-like structure around the southern nucleus. The offset peak position of the H2 emission can be understood if we assume that the shell expanding to the north interacts with the extragalactic molecular gas. At the interface between the shell and the molecular gas concentration the cloud-crushing mechanism proposed by Cowie et al. (1981) may work efficiently, and the intense H2 emission is thus expected there. All these findings lead us to propose a model that the most H2 emission is attributed to the shock excitation driven by the superwind activity of the southern nucleus.
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