INITIAL CONDITIONS FOR STAR FORMATION IN CLUSTERS: PHYSICAL AND KINEMATICAL STRUCTURE OF THE STARLESS CORE Oph A-N6
INITIAL CONDITIONS FOR STAR FORMATION IN CLUSTERS: PHYSICAL AND KINEMATICAL STRUCTURE OF THE STARLESS CORE Oph A-N6
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DOI:
10.1088/0004-637x/745/2/117
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发表时间:
2011-11
期刊:
影响因子:
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通讯作者:
T. Bourke;P. Myers;P. Caselli;J. di Francesco;A. Belloche;R. Plume;D. Wilner
中科院分区:
文献类型:
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作者:
T. Bourke;P. Myers;P. Caselli;J. di Francesco;A. Belloche;R. Plume;D. Wilner
We present high spatial (0.05 over much of the core. The N2H+ column density profile across the major axis of Oph A-N6 is well represented by an isothermal cylinder, with temperature 20 K, peak density 7.1 × 106 cm−3, and N2H+ abundance 2.7 × 10−10. The mass of Oph A-N6 is estimated to be 0.29 M☉, compared to a value of 0.18 M☉ from the isothermal cylinder analysis, and 0.63 M☉ for the critical mass for fragmentation of an isothermal cylinder. Compared to isolated low-mass cores, Oph A-N6 shows similar narrow line widths and small velocity variation, with a deuterium fraction similar to “evolved” dense cores. It is significantly smaller than isolated cores, with larger peak column and volume density. The available evidence suggests that Oph A-N6 has formed through the fragmentation of the Oph A filament and is the precursor to a low-mass star. The dust continuum emission suggests that it may already have begun to form a star.