Direct Three-body Triple-$\alpha$ in Helium Novae

TL;DR

This paper investigates how a revised three-body alpha fusion rate affects helium nova models, finding it extends recurrence times and influences ignition conditions, especially near detonation thresholds.

Contribution

It introduces the impact of the Nguyen et al. (2012) three-body alpha fusion rate on helium nova simulations, highlighting differences from previous resonant rate assumptions.

Findings

Longer recurrence times with the new rate.

Larger ignition masses in nova models.

Potential importance of density increases near detonation thresholds.

Abstract

In AM CVn binaries, a white dwarf primary accretes material from a helium-rich white dwarf or stellar companion. The unstable ignition of nuclear burning via the $3\alpha$ reaction in an accumulated helium layer powers a thermonuclear runaway near accretion rates $\dot{M} \lesssim 10^{-6} \, \mathrm{M_{\odot} \ yr^{-1}}$ that may be observed as helium nova or .Ia supernova. Helium burning in the primary's envelope at temperatures $T \lesssim 10^{8} \, \mathrm{K}$ may proceed via the direct three-body fusion of $\alpha$-particles. Here we show that the direct three-body rate by Nguyen et al. (2012) -- which is reduced relative to the extrapolated resonant rate at temperatures $T \gtrsim 5 \times 10^{7} \, \mathrm{K}$ -- results in novae with longer recurrence times and larger ignition masses. By contrast, we find that the enhancement in the direct three-body rate at temperatures below $T \lesssim 5 \times 10^{7} \, \mathrm{K}$ does not result in significant differences in nova outburst properties. The most massive envelopes in our models are near the density threshold for detonation of the helium layer, where an increase in the density at ignition due to the $3\alpha$ rate may be important.