ABSTRACT Standard stellar evolution theory poorly predicts the surface abundances of chemical species in low-mass, red giant branch (RGB) stars. Observations show an enhancement of p–p chain and CNO cycle products in red giant envelopes, which suggests the existence of non-canonical mixing that brings interior burning products to the surface of these stars. The 12C/13C ratio is a highly sensitive abundance metric used to probe this mixing. We investigate extra RGB mixing by examining: (1) how 12C/13C is altered along the RGB, and (2) how 12C/13C changes for stars of varying age and mass. Our sample consists of 43 red giants, spread over 15 open clusters from the Sloan Digital Sky Survey’s APOGEE DR17, that have reliable 12C/13C ratios derived from their APOGEE spectra. We vetted these 12C/13C ratios and compared them as a function of evolution and age/mass to the standard mixing model of stellar evolution, and to a model that includes prescriptions for RGB thermohaline mixing and stellar rotation. We find that the observations deviate from standard mixing models, implying the need for extra mixing. Additionally, some of the abundance patterns depart from the thermohaline model, and it is unclear whether these differences are due to incomplete observations, issues inherent to the model, our assumption of the cause of extra mixing, or any combination of these factors. Nevertheless, the surface abundances across our age/mass range clearly deviate from the standard model, agreeing with the notion of a universal mechanism for RGB extra mixing in low-mass stars.
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The 3-Helium Problem
The light element 3He is produced in copious amounts during the first three minutes after the Big Bang. The 3He abundance is then modified primarily by nucleosynthesis in stars, whereby low-mass stars (< 2 solar masses) are expected to produce 3He due to the astration of deuterium. The higher temperatues in more massive stars fuse 3He completely into 4He thus destroying 3He. Measurements of 3He are made via observations of the hyperfine transition of 3He+ at 3.46 cm. Observations of 3He+ in HII regions located throughout the Milky Way disk reveal very little variation in the 3He/H abundance ratio — the "3He Plateau", indicating that the net effect of 3He production in stars is negligible. This is in contrast to much higher 3He/H abundance ratios found in some planetary nebula (PNe). This discrepancy is known as the "3He Problem." One solution to this problem is that thermohaline mixing occurs just above the hydrogen-burning shell to process 3-Helium: 3He(3He, 2p)4He. Thermohaline mixing is a double-diffusive instability that occurs in oceans and is also called thermohaline convection. We discuss how more accurate observations of the 3He/H abundance ratio can constrain stellar evolution models that include thermohaline mixing.
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- Award ID(s):
- 1714688
- PAR ID:
- 10342821
- Date Published:
- Journal Name:
- American Astronomical Society meeting #235
- Volume:
- 52
- Issue:
- 1
- Format(s):
- Medium: X
- Sponsoring Org:
- National Science Foundation
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Abstract Thermohaline convection (also known as fingering convection or thermohaline mixing) occurs in stellar radiation zones where a sufficient inversion of the mean molecular weight is present. This process mixes chemicals radially and occurs in a variety of stars, including near the luminosity bump on the red giant branch and potentially in polluted white dwarfs. Previous efforts to characterize this process using 3D simulations have been restricted to regimes far from actual stars: the Prandtl number Pr—the ratio of the kinematic viscosity to thermal diffusivity—assumes values as low as 10−6in stars, but 3D simulations have been restricted to Pr ≳ 10−2. For this reason, disagreements between observations and simulations are routinely dismissed as stemming from this Pr gap. This Letter bridges this gap and demonstrates that 3D simulations of thermohaline convection can be performed in stellar parameter regimes. Using a suite of simulations spanning previously studied regimes with Pr ≳ 10−2down to Pr = 10−6, we demonstrate that the chemical mixing model of J. Brown et al. remains consistent with 3D simulations across both regimes. Therefore, tensions between this model and observations cannot be dismissed as resulting from a Pr gap and must be resolved by considering additional physics.more » « less
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