[Paper Review] Simulating star formation in molecular cores II. The effects of different levels of turbulence
This study uses smoothed particle hydrodynamics (SPH) simulations to investigate how varying levels of initial turbulence in a 5.4 M⊙ molecular core affect star formation, fragmentation, and binary statistics. It finds that a turbulence parameter α_turb ≈ 0.05 best reproduces the observed binary frequency, mass function, and orbital properties of field G-dwarfs, while higher turbulence (α_turb ≥ 0.10) produces a distinct subpopulation of close, comparable-mass binaries consistent with observations in Taurus.
(Abridged) We explore, by means of a large ensemble of SPH simulations, how the level of turbulence affects the collapse and fragmentation of a star-forming core. All our simulated cores have the same, except that we vary (a) the initial level of turbulence (as measured by the ratio of turbulent to gravitational energy, $α_{ m turb} \equiv U_{ m turb}/|Ω| = 0, 0.01, 0.025, 0.05, 0.10 { m and} 0.25$) and (b), for fixed $α_{ m turb}$, the details of the initial turbulent velocity field (so as to obtain good statistics). A low level of turbulence ($α_{ m turb} \sim 0.05$) suffices to produce multiple systems. As $α_{ m turb}$ is increased, the number of objects formed and the companion frequency both increase. The mass function is bimodal, with a flat low-mass segment representing single objects ejected from the core before they can accrete much, and a Gaussian high-mass segment representing objects which because they remain in the core grow by accretion and tend to pair up in multiple systems.
Motivation & Objective
- To determine how different levels of initial turbulence influence the fragmentation, mass function, and binary statistics in collapsing molecular cores.
- To assess whether observed binary characteristics in field G-dwarfs and pre-main sequence stars in Taurus can be reproduced by varying turbulence in core collapse simulations.
- To investigate the role of turbulence in shaping the bimodal mass function and the formation of multiple systems during star formation.
- To compare simulation outcomes with observational data from Duquennoy & Mayor (1991) and White & Ghez (2001) to constrain the turbulence level in cores forming solar-type stars.
- To explore the origin of hard, close binaries with high mass ratios in high-turbulence environments and their consistency with pre-main sequence observations.
Proposed method
- Conduct a large ensemble of smoothed particle hydrodynamics (SPH) simulations of a spherically symmetric 5.4 M⊙ core with a Plummer-like density profile matching L1544 observations.
- Vary the initial turbulent energy relative to gravitational energy via the parameter α_turb = U_turb / |Ω|, testing values: 0, 0.01, 0.025, 0.05, 0.10, and 0.25.
- Generate turbulent velocity fields with a power spectrum P(k) ∝ k⁻⁴ to model observed turbulent substructure in molecular clouds.
- For each α_turb, perform multiple realizations (varying random seeds) to ensure statistical robustness and account for stochasticity in turbulent initial conditions.
- Track the formation, mass growth, ejection, and binary pairing of protostars to derive mass functions and binary statistics (separation, eccentricity, mass ratio).
- Compare simulated binary distributions (semi-major axis, eccentricity, mass ratio) with observational data from Duquennoy & Mayor (1991) and White & Ghez (2001).
Experimental results
Research questions
- RQ1How does the level of initial turbulence (α_turb) affect the number of stars formed and the frequency of multiple systems in collapsing molecular cores?
- RQ2What value of α_turb best reproduces the observed binary frequency, semi-major axis distribution, eccentricity, and mass ratio distribution of field G-dwarfs?
- RQ3Why does a subpopulation of close, high-mass-ratio binaries form at higher turbulence levels (α_turb ≥ 0.10), and is this consistent with observations in Taurus?
- RQ4How does turbulence influence the bimodal structure of the stellar initial mass function, particularly the flat low-mass and Gaussian high-mass segments?
- RQ5Can the observed properties of pre-main sequence binaries in Taurus be reproduced by a mixture of simulations with different α_turb values?
Key findings
- A minimum turbulence level of α_turb ≈ 0.025 is required to form multiple systems, with a ~20% probability of multiple systems forming at this level.
- The observed binary statistics of field G-dwarfs from Duquennoy & Mayor (1991) are best reproduced by simulations with α_turb ≈ 0.05, matching companion frequency, semi-major axis, eccentricity, and mass ratio distributions.
- At α_turb ≥ 0.10, a distinct subpopulation of close binaries with small semi-major axes and high mass ratios (comparable-mass components) emerges, consistent with observations in the Taurus pre-main sequence population.
- The stellar initial mass function is bimodal: a flat low-mass segment from ejected single objects (<0.5 M⊙), and a Gaussian high-mass segment from accreting, embedded multiple systems.
- Approximately 20% of simulated objects are brown dwarfs (M < 0.08 M⊙), and 50% are low-mass stars (0.08 M⊙ < M < 0.5 M⊙), with the latter predominantly forming in multiple systems.
- The mass function and binary statistics of pre-main sequence stars in Taurus are best reproduced by a mix of simulations with α_turb = 0.05 (20 realizations), 0.10 (20 realizations), and 0.25 (10 realizations), as shown in Goodwin et al. (2004b).
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This review was created by AI and reviewed by human editors.