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DETECTION OF POWERFUL MID-IR H2 EMISSION IN THE BRIDGE BETWEEN THE TAFFY GALAXIES
被引:29
作者:
Peterson, B. W.
[1
]
Appleton, P. N.
[2
]
Helou, G.
Guillard, P.
[3
]
Jarrett, T. H.
Cluver, M. E.
[3
,4
]
Ogle, P.
[3
]
Struck, C.
[1
]
Boulanger, F.
[5
]
机构:
[1] Iowa State Univ, Dept Phys & Astron, Ames, IA 50011 USA
[2] CALTECH, IPAC, NASA Herschel Sci Ctr, Pasadena, CA 91125 USA
[3] CALTECH, IPAC, Spitzer Sci Ctr, Pasadena, CA 91125 USA
[4] Australian Astron Observ, Epping, NSW 1710, Australia
[5] Univ Paris 11, Inst Astrophys Spatiale, Orsay, France
基金:
美国国家航空航天局;
关键词:
galaxies:;
individual;
(UGC;
12914;
UGC;
12915);
galaxies: interactions;
intergalactic medium;
SPITZER-SPACE-TELESCOPE;
ULTRALUMINOUS INFRARED GALAXIES;
STAR-FORMATION EFFICIENCY;
WARM MOLECULAR-HYDROGEN;
STEPHANS QUINTET;
NEARBY GALAXIES;
GAS;
SPECTROGRAPH;
REGIONS;
SYSTEM;
D O I:
10.1088/0004-637X/751/1/11
中图分类号:
P1 [天文学];
学科分类号:
0704 ;
摘要:
We report the detection of strong, resolved emission from warm H-2 in the Taffy galaxies and bridge. Relative to the continuum and faint polyclic aromatic hydrocarbon (PAH) emission, the H-2 emission is the strongest in the connecting bridge, approaching L(H-2)/L(PAH 8 mu m) = 0.1 between the two galaxies, where the purely rotational lines of H2 dominate the mid-infrared spectrum in a way very reminiscent of the group-wide shock in the interacting group Stephan's Quintet (SQ). The surface brightness in the 0-0 S(0) and S(1) H-2 lines in the bridge is more than twice that observed at the center of the SQ shock. We observe a warm H2 mass of 4.2 x 10(8) M-circle dot in the bridge, but taking into account the unobserved bridge area, the total warm mass is likely to be twice this value. We use excitation diagrams to characterize the warm molecular gas, finding an average surface mass of similar to 5 x 10(6) M-circle dot kpc(-2) and typical excitation temperatures of 150-175 K. H-2 emission is also seen in the galaxy disks, although there the emission is more consistent with normal star-forming galaxies. We investigate several possible heating mechanisms for the bridge gas but favor the conversion of kinetic energy from the head-on collision via turbulence and shocks as the main heating source. Since the cooling time for the warm H-2 is short (similar to 5000 yr), shocks must be permeating the molecular gas in the bridge region in order to continue heating the H-2.
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页数:15
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