TY - JOUR
T1 - Fates of the dense cores formed by fragmentation of filaments
T2 - Do they fragment again or not?
AU - Sugimura, Kazuyuki
AU - Mizuno, Yurina
AU - Matsumoto, Tomoaki
AU - Omukai, Kazuyuki
N1 - Funding Information:
We would like to thank Gen Chiaki, Shu-ichiro Inutsuka, Kazunari Iwasaki, Sanemichi Takahashi and Toru Tsuribe for fruitful discussions. The numerical simulations were performed on the Cray XC30 at CfCA of the National Astronomical Observatory of Japan. This work is supported in part by MEXT/JSPS KAKENHI Grant Numbers 15J03873 (KS), 26400233, 26287030 and 24244017 (TM) and 25287040 (KO).
Publisher Copyright:
© 2017 The Authors.
PY - 2017/8/1
Y1 - 2017/8/1
N2 - Fragmentation of filaments into dense cores is thought to be an important step in forming stars. The bar-mode instability of spherically collapsing cores found in previous linear analysis invokes a possibility of refragmentation of the cores due to their ellipsoidal (prolate or oblate) deformation. To investigate this possibility, here we perform three-dimensional selfgravitational hydrodynamics simulations that follow all the way from filament fragmentation to subsequent core collapse. We assume that the gas is polytropic with index ? , which determines the stability of the bar mode. For the case that the fragmentation of isolated hydrostatic filaments is triggered by the most unstable fragmentation mode, we find that the bar mode grows as collapse proceeds if < 1.1, in agreement with the linear analysis. However, it takes more than 10 orders-of-magnitude increase in the central density for the distortion to become non-linear. In addition to this fiducial case, we also study non-fiducial ones such as the fragmentation is triggered by a fragmentation mode with a longer wavelength and it occurs during radial collapse of filaments and find that the distortion rapidly grows. In most of astrophysical applications, the effective polytropic index of collapsing gas exceeds 1.1 before 10 orders-of-magnitude increase in the central density. Thus, supposing the fiducial case of filament fragmentation, refragmentation of dense cores would not be likely and their final mass would be determined when the filaments fragment.
AB - Fragmentation of filaments into dense cores is thought to be an important step in forming stars. The bar-mode instability of spherically collapsing cores found in previous linear analysis invokes a possibility of refragmentation of the cores due to their ellipsoidal (prolate or oblate) deformation. To investigate this possibility, here we perform three-dimensional selfgravitational hydrodynamics simulations that follow all the way from filament fragmentation to subsequent core collapse. We assume that the gas is polytropic with index ? , which determines the stability of the bar mode. For the case that the fragmentation of isolated hydrostatic filaments is triggered by the most unstable fragmentation mode, we find that the bar mode grows as collapse proceeds if < 1.1, in agreement with the linear analysis. However, it takes more than 10 orders-of-magnitude increase in the central density for the distortion to become non-linear. In addition to this fiducial case, we also study non-fiducial ones such as the fragmentation is triggered by a fragmentation mode with a longer wavelength and it occurs during radial collapse of filaments and find that the distortion rapidly grows. In most of astrophysical applications, the effective polytropic index of collapsing gas exceeds 1.1 before 10 orders-of-magnitude increase in the central density. Thus, supposing the fiducial case of filament fragmentation, refragmentation of dense cores would not be likely and their final mass would be determined when the filaments fragment.
KW - Galaxies: evolution
KW - Galaxies: star formation
KW - Stars: formation
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U2 - 10.1093/mnras/stx1129
DO - 10.1093/mnras/stx1129
M3 - Article
AN - SCOPUS:85055320044
SN - 0035-8711
VL - 469
SP - 4022
EP - 4033
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
IS - 4
ER -