Abstract

Understanding the origin of stellar masses—the initial mass function (IMF)— remains one of the most challenging problems in astrophysics. The IMF is a key ingredient for simulations of galaxy formation and evolution, and is used to calibrate star formation relations in extra-galactic observations. Modeling the IMF directly in hydrodynamical simulations has been attempted in several previous studies, but the most important processes that control the IMF remain poorly understood. This is because predicting the IMF from direct hydrodynamical simulations involves complex physics such as turbulence, magnetic fields, radiation feedback and mechanical feedback, all of which are difficult to model and the methods used have limitations in terms of accuracy and computational efficiency. Moreover, a physical interpretation of the simulated IMFs requires a numerically converged solution at high resolution, which has so far not been convincingly demonstrated. Here we present a resolution study of star cluster formation aimed at producing a converged IMF. We compare a set of magnetohydrodynamical (MHD) adaptive-mesh-refinement simulations with three different implementations of the thermodynamics of the gas: 1) with an isothermal equation of state (EOS), 2) with a polytropic EOS, and 3) with a simple stellar heating feedback model. We show that in the simulations with an isothermal or polytropic EOS, the number of stars and their mass distributions depend on the numerical resolution. By contrast, the simulations that employ the simple radiative feedback module demonstrate convergence in the number of stars formed and in their IMFs.

Highlights

  • The IMF is the distribution of stellar masses when they are born

  • The simulations that include stellar heating feedback show convergence, with 28 and 29 sink particles formed in the low- and high-resolution simulations, respectively

  • Summary and conclusions We implemented a new simple stellar heating module in the FLASH MHD code (§3). This heating feedback module takes the luminosity of a protostar or evolved star and distributes the radiated energy in a spherically symmetric approximation around each star

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Summary

Introduction

The IMF is the distribution of stellar masses when they are born. We know from observational surveys that most stars have masses of about half the mass of our Sun (M ). The highmass tail of the IMF is a steeply decreasing power-law function with the number of stars N (M ) ∝ M −1.35 [1, 2, 3, 4, 5, 6, 7, 8]. Understanding this seemingly universal power-law tail and the turnover at around 0.5 M is one of the most challenging open problems in astrophysics. The IMF has far-reaching consequences and applications, e.g., for calibrating extra-galactic star formation relations used to understand galaxy formation and evolution

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