Abstract

The triple-alpha process, whereby evolved stars create carbon and oxygen, is believed to be fine-tuned to a high degree. Such fine-tuning is suggested by the unusually strong temperature dependence of the triple-alpha reaction rate at stellar temperatures. This sensitivity is due to the resonant character of the triple-alpha process, which proceeds through the so-called “Hoyle state” of {}^{12}mathrm{C} with spin-parity 0^+. The question of fine-tuning can be studied within the ab initio framework of nuclear lattice effective field theory, which makes it possible to relate ad hoc changes in the energy of the Hoyle state to changes in the fundamental parameters of the nuclear Hamiltonian, which are the light quark mass m_q and the electromagnetic fine-structure constant alpha _mathrm{em}. Here, we update the effective field theory calculation of the sensitivity of the triple-alpha process to small changes in the fundamental parameters. In particular, we consider recent high-precision lattice QCD calculations of the nucleon axial coupling g_A, as well as new and more comprehensive results from stellar simulations of the production of carbon and oxygen. While the updated stellar simulations allow for much larger ad hoc shifts in the Hoyle state energy than previously thought, recent lattice QCD results for the nucleon S-wave singlet and triplet scattering lengths now disfavor the “no fine-tuning scenario” for the light quark mass m_q.

Highlights

  • Known as the Hoyle state [1]

  • We review here how the sensitivity of the triple-alpha reaction rate with respect to small changes in the light quark mass and the electromagnetic fine-structure constant is treated in the effective field theory (EFT) framework

  • We contrast this theoretical treatment with recent high-precision calculations of stellar nucleosynthesis, which find that the allowable range of Hoyle state energies is larger than previously thought [3]

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Summary

Introduction

This paper is structured as follows: In Sect. 2, we update the pion (or quark) mass dependence of the nuclear Hamiltonian, which is central for the discussion which follows. This paper is structured as follows: In Sect. 2, we update the pion (or quark) mass dependence of the nuclear Hamiltonian, which is central for the discussion which follows. 3, we review the current status of stellar nucleosynthesis calculations, with focus on the resulting abundances of carbon and oxygen under ad hoc shifts in the Hoyle state resonance. We pay attention to recent new results in this field. 4, we revisit the theoretical status of

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Quark mass dependence of the nuclear Hamiltonian
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The Hoyle state in stellar nucleosynthesis
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Sensitivity to small changes in the fundamental parameters
Discussion
Findings
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