2018MNRAS.480.1043N


Query : 2018MNRAS.480.1043N

2018MNRAS.480.1043N - Mon. Not. R. Astron. Soc., 480, 1043-1056 (2018/October-2)

Condition for low-mass star formation in shock-compressed metal-poor clouds.

NAKAUCHI D., OMUKAI K. and SCHNEIDER R.

Abstract (from CDS):

Shocks may have been prevalent in the early Universe, associated with virialization and supernova explosions, etc. Here, we study thermal evolution and fragmentation of shock-compressed clouds, by using a one-zone model with detailed thermal and chemical processes. We explore a large range of initial density (1-105 cm–3), metallicity (0-10–2 Z☉), UV strength (0-500 times Galactic value), and cosmic microwave background temperature (10 and 30 K). Shock-compressed clouds contract isobarically via atomic and molecular line cooling, until self-gravitating clumps are formed by fragmentation. If the metals are only in the gas-phase, the clump mass is higher than ∼3 M☉ in any conditions we studied. Although in some cases with a metallicity higher than ∼10–3 Z☉, re-fragmentation of a clump is caused by metal-line cooling, this fragment mass is higher than ∼30 M☉. On the other hand, if about half the mass of metals is condensed in dust grains, as in the Galactic interstellar medium, dust cooling triggers re-fragmentation of a clump into subsolar mass pieces, for metallicities higher than ∼10–5 Z☉. Therefore, the presence of dust is essential in low-mass (<= M☉) star formation from a shock-compressed cloud.

Abstract Copyright: © 2018 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): stars: formation - stars: Population III - stars: Population II

Errata: erratum vol. 483, p. 1265 (2019)

Simbad objects: 2

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Number of rows : 2
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 SDSS J002314.00+030758.0 * 00 23 14.0027073768 +03 07 58.241752572           A2II 28 0
2 UCAC3 215-112497 Pe* 10 29 15.1489854864 +17 29 27.924626724   17.424 16.708   15.98 sdA 120 0

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