Identify why a 1.1 M_sun C/O white dwarf with 10^{-3} M_sun added helium fails to detonate despite l_sonic < H_P
Ascertain the mechanism that prevents a helium shell detonation from propagating in the simulated 1.1 solar-mass carbon–oxygen white dwarf after the addition of 10^{-3} solar masses of helium-rich material and relaxation—even though the local condition l_sonic < H_P at the transition layer is satisfied—and determine what additional factors (e.g., compositional structure, thermal profile, geometry, or numerical treatment) necessitate ≥2×10^{-3} solar masses of added helium for successful shell and core detonations.
References
For reasons that are unclear, an additional $ \geq 2#1{-3} $ is required for a shell and core detonation for the $1.1 $ model, even though $l_{\rm sonic} < H_P$ is achieved for the $1.1 + 10{-3} $ case. Further investigation is required to understand why a detonation does not propagate in this case.
Reactions are not coupled to hydrodynamics and the composition is not evolved, so we cannot say if the burning would spread beyond the candidate material.