TY - JOUR
T1 - The role of the H2 adiabatic index in the formation of the first stars
AU - Sharda, Piyush
AU - Krumholz, Mark R.
AU - Federrath, Christoph
N1 - Publisher Copyright:
© 2019 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society
PY - 2019/11/21
Y1 - 2019/11/21
N2 - The adiabatic index of H2 (γH2 ) is non-constant at temperatures between 100 and 104 K due to the large energy spacing between its rotational and vibrational modes. For the formation of the first stars at redshifts 20 and above, this variation can be significant because primordial molecular clouds are in this temperature range due to the absence of efficient cooling by dust and metals. We study the possible importance of variations in γH2 for the primordial initial mass function by carrying out 80 3D gravitohydrodynamic simulations of collapsing clouds with different random turbulent velocity fields, half using fixed γH2 = 7/5 in the limit of classical diatomic gas (used in earlier works) and half using an accurate quantum mechanical treatment of γH2 . We use the adaptive mesh refinement code FLASH with the primordial chemistry network from KROME for this study. The simulation suite produces almost 400 stars, with masses from 0.02 to 50 M (mean mass ∼10.5 M and mean multiplicity fraction ∼0.4). While the results of individual simulations do differ when we change our treatment of γH2 , we find no statistically significant differences in the overall mass or multiplicity distributions of the stars formed in the two sets of runs. We conclude that, at least prior to the onset of radiation feedback, approximating H2 as a classical diatomic gas with γH2 = 7/5 does not induce significant errors in simulations of the fragmentation of primordial gas. None the less, we recommend using the accurate formulation of the H2 adiabatic index in primordial star formation studies since it is not computationally more expensive and provides a better treatment of the thermodynamics.
AB - The adiabatic index of H2 (γH2 ) is non-constant at temperatures between 100 and 104 K due to the large energy spacing between its rotational and vibrational modes. For the formation of the first stars at redshifts 20 and above, this variation can be significant because primordial molecular clouds are in this temperature range due to the absence of efficient cooling by dust and metals. We study the possible importance of variations in γH2 for the primordial initial mass function by carrying out 80 3D gravitohydrodynamic simulations of collapsing clouds with different random turbulent velocity fields, half using fixed γH2 = 7/5 in the limit of classical diatomic gas (used in earlier works) and half using an accurate quantum mechanical treatment of γH2 . We use the adaptive mesh refinement code FLASH with the primordial chemistry network from KROME for this study. The simulation suite produces almost 400 stars, with masses from 0.02 to 50 M (mean mass ∼10.5 M and mean multiplicity fraction ∼0.4). While the results of individual simulations do differ when we change our treatment of γH2 , we find no statistically significant differences in the overall mass or multiplicity distributions of the stars formed in the two sets of runs. We conclude that, at least prior to the onset of radiation feedback, approximating H2 as a classical diatomic gas with γH2 = 7/5 does not induce significant errors in simulations of the fragmentation of primordial gas. None the less, we recommend using the accurate formulation of the H2 adiabatic index in primordial star formation studies since it is not computationally more expensive and provides a better treatment of the thermodynamics.
KW - Early Universe
KW - Hydrodynamics
KW - Primordial nucleosynthesis
KW - Stars: Population III
KW - Stars: formation
KW - Turbulence
UR - http://www.scopus.com/inward/record.url?scp=85075242757&partnerID=8YFLogxK
U2 - 10.1093/mnras/stz2618
DO - 10.1093/mnras/stz2618
M3 - Article
SN - 0035-8711
VL - 490
SP - 513
EP - 526
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
IS - 1
ER -