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THE STELLAR AND GAS KINEMATICS OF THE LITTLE THINGS DWARF IRREGULAR GALAXY NGC 1569

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Citations

64

References

2012

Year

Abstract

In order to understand the formation and evolution of dIm galaxies, one needs\nto understand their three-dimensional structure. We present measurements of the\nstellar velocity dispersion in NGC 1569, a nearby post-starburst dIm galaxy.\nThe stellar vertical velocity dispersion, $\\sigma_{\\rm z}$, coupled with the\nmaximum rotational velocity derived from \\ion{H}{1} observations, $V_{\\rm\nmax}$, gives a measure of how kinematically hot the galaxy is, and, therefore,\nindicates its structure. We conclude that the stars in NGC 1569 are in a thick\ndisk with a $V_{\\rm max} / \\sigma_{\\rm z}$ = 2.4 $\\pm$ 0.7. In addition to the\nstructure, we analyze the ionized gas kinematics from \\ion{O}{3} observations\nalong the morphological major axis. These data show evidence for outflow from\nthe inner starburst region and a potential expanding shell near supermassive\nstar cluster (SSC) A. When compared to the stellar kinematics, the velocity\ndispersion of the stars increase in the region of SSC A supporting the\nhypothesis of an expanding shell. The stellar kinematics closely follow the\nmotion of the gas. Analysis of high resolution \\ion{H}{1} data clearly reveals\nthe presence of an \\ion{H}{1} cloud that appears to be impacting the eastern\nedge of NGC 1569. Also, an ultra-dense \\ion{H}{1} cloud can be seen extending\nto the west of the impacting \\ion{H}{1} cloud. This dense cloud is likely the\nremains of a dense \\ion{H}{1} bridge that extended through what is now the\ncentral starburst area. The impacting \\ion{H}{1} cloud was the catalyst for the\nstarburst, thus turning the dense gas into stars over a short timescale, $\\sim$\n1 Gyr. We performed a careful study of the spectral energy distribution using\ninfrared, optical, and ultraviolet photometry producing a state-of-the-art mass\nmodel for the stellar disk. This mass modeling shows that stars dominate the\ngravitational potential in the inner 1 kpc.\n

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