Issue 
A&A
Volume 633, January 2020



Article Number  A23  
Number of page(s)  15  
Section  Stellar structure and evolution  
DOI  https://doi.org/10.1051/00046361/201936666  
Published online  24 December 2019 
Chemical mixing in low mass stars
I. Rotation against atomic diffusion including radiative acceleration
^{1}
Instituto de Astrofísica e Ciências do Espaço, Universidade do Porto CAUP, Rua das Estrelas, 4150762 Porto, Portugal
email: morgan.deal@astro.up.pt
^{2}
LESIA, Observatoire de Paris, Université PSL, CNRS, Sorbonne Université, Université de Paris, 5 Place Jules Janssen, 92195 Meudon, France
^{3}
Institut d’Astrophysique Spatiale, UMR8617, CNRS, Université ParisSaclay, Bâtiment 121, 91405 Orsay Cedex, France
^{4}
Univ. Rennes, CNRS, IPR (Institut de Physique de Rennes) – UMR 6251, 35000 Rennes, France
Received:
10
September
2019
Accepted:
31
October
2019
Context. When modelling stars with masses higher than 1.2 M_{⊙} with no observed chemical peculiarity, atomic diffusion is often neglected because, on its own, it causes unrealistic surface abundances compared with those observed. The reality is that atomic diffusion is in competition with other transport processes. Rotation is one of the processes able to prevent excessively strong surface abundance variations.
Aims. The purpose of this study is to quantify the opposite or conjugated effects of atomic diffusion (including radiative acceleration) and rotationally induced mixing in stellar models of low mass stars, and to assess whether rotational mixing is able to prevent the strong abundance variations induced by atomic diffusion in Ftype stars. Our second goal is to estimate the impact of neglecting both rotational mixing and atomic diffusion in stellar parameter inferences for stars with masses higher than 1.3 M_{⊙}.
Methods. Using the Asteroseismic Inference on a Massive Scale (AIMS) stellar parameter inference code, we infer the masses and ages of a set of representative artificial stars for which models were computed with the Code d’Evolution Stellaire Adaptatif et Modulaire (CESTAM; the T stands for Transport) evolution code, taking into account rotationally induced mixing and atomic diffusion, including radiative acceleration. The observed constraints are asteroseismic and classical properties. The grid of stellar models used for the optimization search include neither atomic diffusion nor rotationally induced mixing. The differences between real and retrieved parameters then provide an estimate of the errors made when neglecting transport processes in stellar parameter inference.
Results. We show that for masses lower than 1.3 M_{⊙}, rotation dominates the transport of chemical elements and strongly reduces the effect of atomic diffusion, with net surface abundance modifications similar to solar values. At higher mass, atomic diffusion and rotation are competing equally. Above 1.44 M_{⊙}, atomic diffusion dominates in stellar models with initial rotation lower than 80 km s^{−1} producing a chemical peculiarity which is not observed in Kepler Legacy stars. This indicates that a transport process of chemical elements is missing, probably linked to the missing transport process of angular momentum needed to explain rotation profiles in solarlike stars. Importantly, neglecting rotation and atomic diffusion (including radiative acceleration) in the models, when inferring the parameters of Ftype stars, may lead to respective errors of ≈5%, ≈2.5%, and ≈25% for stellar masses, radii, and ages.
Conclusions. Atomic diffusion (including radiative acceleration) and rotational mixing should be taken into account in stellar models in order to determine accurate stellar parameters. When atomic diffusion and shellular rotation are both included, they enable stellar evolution codes to reproduce the observed metal and helium surface abundances for stars with masses up to 1.4 M_{⊙} at solar metallicity. However, if rotation is actually uniform for these stars (as observations seem to indicate), then an additional chemical mixing process is needed together with a revised formulation of rotational mixing. For higher masses, an additional mixing process is needed in any case.
Key words: stars: interiors / diffusion / stars: rotation / stars: evolution / asteroseismology / stars: solartype
© ESO 2019
1. Introduction
The determination of stellar classical parameters (such as age, mass, and radius) is possible through the computation of stellar models. These models depend on micro and macrophysics input ingredients and can be constrained thanks to spectroscopic, astrometric, photometric, interferometric, and asteroseismic observations. Of these, asteroseismology is the only one that can give information on the internal structure of stars; the others only give access to surface layers.
In order to reproduce all available observations, the physical processes at work in the stellar plasma have to be identified and, if recognized as efficient, have to be taken into account in stellar models. This can imply a heavy computational cost, but it is a necessary step towards the determination of stellar parameters that are as accurate as possible. In this respect, chemical element transport in stellar interiors is a key ingredient. While macroscopic transport by convection was recognized as a major process a long time ago, microscopic transport due to gravitational settling was considered to be a crucial transport process only after helioseismology placed constraints on the solar sound speed profile (ChristensenDalsgaard et al. 1993).
Transport processes of chemical elements are of two types: microscopic (hereafter atomic diffusion) and macroscopic. The origin of atomic diffusion comes from the first principles of physics and is a direct consequence of the fact that stars are selfgravitating spheres of plasma composed of different gases (chemical element mixture). The equilibrium of stars leads to internal gradients of pressure, temperature, density, and radiative transfer producing a selective motion of chemical elements. Atomic diffusion is mainly led by the competition between gravity, which makes the elements move towards the centre of the star, and radiative acceleration, which is due to the transfer of momentum between photons and ions and makes the elements move towards the surface. The combination of the two processes leads either to a local depredion of elements or to an accumulation, the net effect depending on the chemical element under consideration.
Macroscopic transport processes are plasma instabilities that induce the transport of chemical elements on a large scale. Most of the time these processes are treated as diffusive and are in direct competition with atomic diffusion. This competition occurs for all types of stars and at each evolutionary stage. The result of this competition depends on the relative timescales of all possible processes. The timescale of atomic diffusion for stars with masses close to the solar value is long (5–10 Gyr) and decreases for more massive stars (up to a dozen Myr for A and Btype stars). Depending on the competing transport processes, the variations of the surface abundances are different. If the atomic diffusion timescale is longer or shorter than that of a competing transport process, then the surface abundances remain close to the birth composition of the star. This is the case of the Sun where a 10% depredion of helium and metals is observed (Bahcall & Pinsonneault 1992; Bahcall et al. 1995; ChristensenDalsgaard et al. 1996; Richard et al. 1996; Ciacio et al. 1997; Gabriel 1997; Morel 1997; Brun et al. 1998; Elliott 1998; Turcotte et al. 1998a). In other cases when the atomic diffusion timescale is short, surface abundances can be very different from the initial values, as in chemically peculiar stars (e.g. Praderie 1967; Michaud 1970; Watson 1970, 1971; Richer et al. 2000; Richard et al. 2001; Michaud et al. 2011; Deal et al. 2016). In standard models the only macroscopic transport process included is convection. In convective zones the mixing of chemical elements is very efficient and we can consider atomic diffusion to be negligible, but convection alone is not enough to explain the surface abundances of observed stars. It is then mandatory to include nonstandard processes; one of the most studied ones is the mixing of chemical elements induced by the rotation of the star.
Michaud (1982) first quantified the competition between atomic diffusion and meridional circulation in the envelopes of AmFm stars. Twodimensional simulations of this competition were carried out by Charbonneau & Michaud (1988, 1991). These authors assumed a quasisolid body rotation and an advective transport of chemical elements by meridional circulation (Tassoul & Tassoul 1982). They concluded that AmFm stars can exist if rotation is slower than 100 km s^{−1}, meaning that in these stars atomic diffusion is the dominant transport process. It is worth pointing out that AmFm stars are at the border of the solarlike oscillating star (K7F5) domain that we consider in this work.
Rotation is often invoked as the process that prevents atomic diffusion from having a significant impact on stars as it is able to efficiently transport chemical elements. The first aim of the present work is to check whether this assertion is valid for masses in the range [1.3;1.44] M_{⊙} on the main sequence. To this end, we built stellar models consistently taking into account both processes as they are currently modelled. We examined how different levels of rotation can counteract atomic diffusion processes. We first compared models of virtual stars and then examined how, in real stars, the different effects can be evidenced on the basis of observational constraints.
Asteroseismology allows us to probe the structure of stars. In particular, asteroseismic studies have demonstrated that atomic diffusion has an impact on the inner structure of stars (see e.g. Deal et al. 2017, 2018). Eggenberger et al. (2010) investigated the combined impact of rotation and atomic diffusion for 1 M_{⊙} models. The authors show for instance that rotation by counteracting atomic diffusion keeps the surface helium from decreasing significantly compared with the case of nonrotating models. Some effects on specific seismic diagnostics nevertheless exist due to the structural differences between models without rotation and those with rotation and atomic diffusion. As we show here, this remains true as long as the impact of rotation dominates over the impact of atomic diffusion, that is for stars with low masses. It is then necessary to quantify the impact of atomic diffusion on the stellar parameter determination for stars with increasing masses.
The combined effect of atomic diffusion including radiative acceleration and rotational transport on star surface abundances and internal structures has never been studied in the light of the very precise asteroseismic data currently available from Kepler, and the new generation of stellar models including atomic diffusion and the effect of rotation. We use the Code d’Evolution Stellaire Adaptatif et Modulaire (CESTAM, the T stands for Transport) evolution code (Morel & Lebreton 2008; Marques et al. 2013; Deal et al. 2018), which is one of the few evolution codes, together with the Toulouse Geneva Evolution Code (TGEC) (HuiBonHoa 2008; Théado et al. 2012) and Modules for Experiments in Stellar Astrophysics (MESA) (Paxton et al. 2018), able to compute such models selfconsistently. The errors on the stellar parameter inference when we neglect rotation and/or atomic diffusion are then estimated using the Asteroseismic Inference on a Massive Scale (AIMS) stellar model optimization pipeline (Rendle et al. 2019).
The second goal of the present paper is to assess the net result of atomic diffusion (including radiative acceleration) and rotationally induced mixing on the surface abundance and stellar parameter determination of solarlike oscillating stars with masses below 1.5 M_{⊙}. Stellar models were built for this purpose and are described in Sect. 2. The impact of atomic diffusion and rotation on the transport of chemical elements is presented in Sect. 3. The method we used to infer the stellar parameters and the associated grid of models is described in Sect. 4. Then the results of optimizations are presented in Sect. 5. Finally, we discuss the results and conclude in Sect. 6.
2. Stellar models
We computed stellar models with the CESTAM evolution code (Morel & Lebreton 2008; Marques et al. 2013). We focused on the interval of mass where the effect of radiative acceleration is important (between 1.3 and 1.44 M_{⊙}Deal et al. 2018) and where the efficiency of the transport of chemical elements by rotation is decreasing (e.g. Talon 2008). In this exploratory work, due to the substantial amount of computational time needed, we only consider models at solar metallicity.
2.1. Input physics, including atomic diffusion
In this study the important input physics are atomic diffusion; also important are opacities, which are affected by the modification of chemical mixture induced by diffusion.
Atomic diffusion was computed following the Michaud & Proffitt (1993) formalism and the singlevalued approximation (LeBlanc & Alecian 2004) for radiative acceleration. Details on the atomic diffusion computation in CESTAM are given in Deal et al. (2018). The elements and isotopes that are followed are ^{1}H, ^{3}He, ^{4}He, ^{12}C, ^{13}C, ^{14}N, ^{15}N, ^{15}O, ^{16}O, ^{17}O, ^{22}Ne, ^{23}Na, ^{24}Mg, ^{27}Al, ^{28}Si, ^{31}P (without radiative acceleration), ^{32}S, ^{40}Ca, and ^{56}Fe.
Rigourously speaking, the Rosseland mean opacities should be computed for the exact variation of the chemical mixture at each mesh point in the star and each evolution time step. We then could use the OPCD3 package provided by the Opacity Project^{1}. However, such opacity calculations are excessively time consuming. Therefore, we restricted the full computation of opacity with OPCD3 to the interval T ∈ [10^{4}, 10^{6.23}] K. In this temperature range we found that the contribution to opacity of the elements that vary the most due to atomic diffusion (mainly iron here) is important. This requires a detailed opacity calculation for the exact associated chemical mixture. On the other hand, in the regions where T > 10^{6.23} K and T < 10^{4} K, the initial solar mixture is only slightly affected by atomic diffusion and the impact on opacity can safely be neglected. There we used the opacity tables of the Opacity Project (OP, Seaton 2005) and the Wichita opacity data (Ferguson et al. 2005), respectively. We checked that the opacity smoothly varies at the boundaries of the different tables. Both sets of tables correspond to a fixed solar mixture, the Asplund et al. (2009) mixture with meteoritic abundances for refractory elements recommended by Serenelli (2010).
Convection is treated following the Canuto et al. (1996) prescription. The mixinglength parameter is calibrated so that the solar model reaches the solar radius and luminosity at solar age which yields α_{CGM} = 0.68 (see e.g. Lebreton & Goupil 2014) for models with atomic diffusion and without rotation. We chose to keep this value for all the models of the study in order to assess the impact of the sole physical process under study. We discuss this point in Sect. 5.5.
Other input physics are the same as used by Lebreton & Goupil (2014). Briefly, we used the OPAL2005 equation of state (Rogers & Nayfonov 2002) and nuclear reactions rates from the NACRE compilation (Angulo 1999) except for the ^{14}N(p, γ)^{15}O reaction, for which we use the LUNA rate (Imbriani et al. 2004). Atmospheres are computed in the grey approximation and integrated up to an optical depth of τ = 10^{−4}, and we do not consider mass loss.
2.2. Rotational mixing
Rotationally induced transport as implemented in CESTAM is detailed in Marques et al. (2013). The transport of angular momentum obeys the advectiondiffusion equation
where ρ is the density, r is the local radius, Ω the mean angular velocity at radius r, U_{2} the vertical component of meridional circulation velocity at radius r, and ν_{v} the vertical component of the turbulent viscosity.
When angular momentum loss is taken into account at the surface, we use the prescription of Matt et al. (2015) for magnetized wind braking with a solar calibrated constant of 1.25 × 10^{31} erg (except in the uniform rotation case, see Sect. 3.2). Models are computed from the zero age main sequence (ZAMS) with an initial surface rotation of either 30 km s^{−1} or 80 km s^{−1} to cover the range of rotation speed observed for Kepler stars showing detectable solarlike oscillation frequencies.
The vertical component of the turbulent diffusivity is given by (Chaboyer & Zahn 1992; Talon & Zahn 1997)
where Ri_{c} = 1/6 is the critical Richardson number, K the thermal diffusivity, N_{T} and N_{μ} the chemical and thermal parts of the Brunt–Väisälä frequency, and D_{h} the horizontal component of turbulent diffusivity. For D_{h}, we used the prescription of Mathis et al. (2004):
Here V_{2} and U_{2} are the horizontal and vertical components of the velocity of the meridional circulation, and β = 1.5 × 10^{−5} (Richard & Zahn 1999). We assumed that the vertical turbulent diffusivity D_{V} is equal to the vertical turbulent viscosity ν_{V}.
The combination of the transport of chemical elements by meridional circulation and horizontal turbulence results in a diffusive process with a coefficient given by Chaboyer & Zahn (1992):
The total diffusion coefficient of chemical elements associated with rotation is then given by
This formalism for transport of angular momentum was used to compute the evolution of the rotation profile of stellar models for solarlike oscillating stars. The seismic diagnostics associated with the resulting rotation profiles were then compared with the observational data (e.g. Eggenberger et al. 2012; Marques et al. 2013). It was shown to be too inefficient to account for the internal rotation inferred from observed stars (e.g. Deheuvels et al. 2012; Aerts et al. 2019; Ouazzani et al. 2019; Buldgen 2019) despite various efforts to improve it (see e.g. Mathis et al. 2018). The purpose of the present paper is not to reproduce real stars, but rather to understand the interaction between microscopic and macroscopic aspects of the transport. It is a step torward a more detailed and accurate theory for the transport of chemical elements in stars. Nevertheless we also investigate the case when a uniform rotation is imposed during the evolution of the stellar models.
2.3. Coupling between atomic diffusion and rotational mixing
The interaction between rotation and atomic diffusion occurs at different levels. One of them is the impact of the μgradient on the meridional circulation (e.g. Charbonnel et al. 1998) which is not discussed in this study. We focus instead on the most obvious one that is the direct competition between atomic diffusion and turbulent diffusion (see Eq. (5)). This coupling clearly appears in the diffusion equation:
Here X_{i} is the mass fraction of element i, v_{i} its atomic diffusion velocity, ρ the density in the considered layer, D_{turb, rota} the turbulent diffusion coefficient, A_{i} its atomic mass, m_{p} the mass of a proton, and r_{ij} the reaction rate of the reaction that transforms element i into j.
In the case of a trace element i, v_{i} can be expressed as
where D_{ip} is the diffusion coefficient of element i relative to protons. The variable g_{rad, i} is the radiative acceleration on element i, g the local gravity, the average charge (in proton charge units) of element i (roughly equal to the charge of the dominant ion), k the Boltzmann constant, T the temperature, and κ_{T} the thermal diffusivity.
Regarding Eq. (6), we can define three regimes:

, when the rotation is strong enough to significantly reduce the effect of atomic diffusion;

, when rotation and atomic diffusion are of the same order of magnitude;

, when the rotation is not able to significantly reduce the effect of atomic diffusion.
As is shown in next section, the three regimes are encountered in solarlike oscillating mainsequence stars. The value of D_{turb, rota}, and therefore the efficiency of the rotationally induced mixing, depends mainly on the value of D_{v} as D_{h} ≫ (rU_{2})^{2}/30 in all the models considered in this study (see Eq. (5)). On the other hand, D_{v} mainly depends on the angular momentum gradient (Eq. (2)). Hence rotation has a strong impact on the transport of chemical elements when the rotation velocity is high or when the gradient of angular momentum is large, for example at the bottom of the surface convective zone. In the other regimes the effect of rotation is negligible or of the same order of magnitude as atomic diffusion.
The presence of an angular momentum gradient at the bottom of a stellar surface convective zone and the associated mixing of chemical elements then depend on how well the meridional circulation is driven. In the case when the total angular momentum is conserved, the efficiency of meridional circulation and the associated transport of chemical elements decrease rapidly with time. One of the few processes able to maintain meridional circulation efficiently on the main sequence is the extraction of angular momentum at the surface during the evolution. This extraction produces a gradient of angular momentum that drives the meridional circulation (increasing the U_{2} term), and then increases the vertical transport of angular momentum. This increase in the angular momentum transport leads to an important mixing of chemical elements able to significantly reduce atomic diffusion.
The most studied extraction of angular momentum at the surface of stars is the extraction through magnetized winds. Several empirical and theoretical prescriptions exist to model this extraction (e.g. Skumanich 1972; Kawaler 1988; Matt et al. 2012, 2015). This extraction is efficient for a star able to maintain a magnetic field generated by a dynamo. The star then needs a surface convective zone large enough to generate these fields. This is why the extraction of angular momentum due to magnetized winds is very efficient for stars with masses lower than 1.2 M_{⊙} at solar metallicity. The efficiency is lower when the mass of the star is higher (i.e. when the size of the surface convective zone is smaller). This is what explains the hot part of the lithium dip (e.g. Talon 2008).
On the other hand, in regions of the star where radiative acceleration is efficient, atomic diffusion produces accumulations of elements. Accumulation of a chemical element occurs in layers where this element significantly contributes to the opacity. It results in a local increase in the opacity. In solarlike oscillating mainsequence stars the accumulation occurs at the surface, which induces an increase in the size of the surface convection zone (Turcotte et al. 1998b; Deal et al. 2017, 2018). This in turn increases the efficiency of the extraction through magnetized wind and the mixing of chemical elements, but at the same time the extraction of angular momentum makes the star rotate more slowly, decreasing the efficiency of mixing of chemical elements. The net result can therefore significantly differ from one star to another depending on its mass and evolutionary state.
In the next section we illustrate this rotationatomic diffusion interaction process with stellar evolution models computed with the current physical description of both rotation and atomic diffusion in a consistent way.
3. Net mixing induced by rotation and atomic diffusion
3.1. Surface abundances
We showed in Deal et al. (2018) that the abundance variations produced by atomic diffusion alone can be very large and may not reproduce observations. This is so because atomic diffusion does not occur alone in stars. There are other processes that are in competition with atomic diffusion and reduce its effects. Rotational mixing is one of them. Therefore, here we aim to determine whether the surface abundances of solarlike oscillating mainsequence stars can be reproduced in models, simultaneously including atomic diffusion and rotationally induced mixing. To answer this question we computed stellar models with the characteristics listed in Table 1. We considered three values of the mass, 1.3, 1.4, and 1.44 M_{⊙} respectively for models A, B, and C, which are found to correspond to the three regimes mentioned in Sect. 2.3. The reference models (A1, B1, B2, C1, and C2) include rotationally induced mixing with two initial values of the rotation velocity, atomic diffusion with radiative acceleration, and extraction of angular momentum at the surface. We point out that the mixing induced by rotation is strong enough to prevent numerical instabilities produced by radiative acceleration. We therefore do not have to impose an ad hoc mixing at the base of the convective zone as is otherwise usually done (Théado et al. 2009; Deal et al. 2016, 2018).
Inputs of the stellar models.
3.1.1. Impact of the initial rotational velocity
Measured surface rotation rates of solarlike stars do not exceed 35 km s^{−1} (e.g. Benomar et al. 2015). We concentrate on surface initial rotation velocities between 30 and 80 km s^{−1} in order to characterize the impact of atomic diffusion and rotation on stars that were observed (Kepler, TESS) or will be observed (PLATO) for asteroseismology.
Figure 1 shows the temporal evolution of the surface abundance of some elements (iron, helium, and carbon). As an observed seismic proxy for the age, we use ν_{max}, the frequency at maximum power in the oscillation spectrum of solarlike pulsators. The value of ν_{max} indeed decreases as stars evolve on the main sequence (Brown 1991; Kjeldsen & Bedding 1995; Kallinger et al. 2010). Regarding the models, we can identify three regimes (as presented in Sect. 2.3):
Fig. 1. Evolution of the surface [Fe/H] in dex (top panel), helium Y_{Surf} in mass fraction (middle panel), and the surface [C/H] in dex (lower panel) as a function of ν_{max} for different masses and initial rotation speeds for models including atomic diffusion with radiative acceleration. Horizontal dotted lines represent the initial abundance. The models are A1, B1, B2, C1, and C2 from Table 1. 

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– For masses lower than 1.4 M_{⊙} (illustrated by model A1 in Fig. 1), we find that the effect of atomic diffusion is small compared with that of rotation. In this mass range, the extraction of angular momentum by the magnetized wind is efficient because the surface convective zone is still thick enough to maintain a dynamo. Meridional circulation is then still efficiently driven, and is able to maintain differential rotation. This induces a relatively strong mixing which prevents unrealistic chemical element depredions due to atomic diffusion. Accordingly, the surface abundance depredions are small and comparable to the values observed in the Sun (e.g. Bahcall & Pinsonneault 1992). The helium and metal surface abundances resulting from the competition between atomic diffusion and rotation are compatible with observations (Ghazaryan et al. 2018; Verma et al. 2019), in particular the helium surface mass fraction Y_{s} always remains higher than 0.18.
We note that even in this case the surface abundances vary with time. The surface variations are similar in the two models of 1.3 M_{⊙} with initial rotation velocities of 30 km s^{−1} and 80 km s^{−1} (the latter, model A2, is not shown in Fig. 1).
– For stars with masses around 1.4 M_{⊙} (see models B1 and B2 in Fig. 1), we find that atomic diffusion and rotation are equally important. Rotation prevents atomic diffusion from inducing large depredions or accumulations of metals and helium at the surface. Atomic diffusion still induces an iron depredion of 0.1 dex, which is of the order of magnitude of the observed surface abundance uncertainties. Helium reaches a depredion level that is still consistent with observations (Ghazaryan et al. 2018; Verma et al. 2019). The initial rotation speed starts to have an effect on the surface abundances variations, but this effect remains too small to be observed.
– For stars with masses higher than 1.4 M_{⊙} (C1 and C2 models in Fig. 1), we find that atomic diffusion dominates over rotation in the studied range of initial rotation speeds. Iron accumulation occurs at the surface, while helium and carbon are strongly depreded. While the iron surface abundance is still compatible with observations, helium is too depreded (Ghazaryan et al. 2018; Verma et al. 2019). The effect of the initial rotation speed is now clearly visible in Fig. 1, with a 0.1 dex decrease in the iron enhancement when rotation increases from 30 to 80 km s^{−1}. In this case the surface convective zone is thin (log(ΔM/M^{*})≈ − 6)), and an efficient dynamo cannot be maintained. This results in a less efficient extraction of angular momentum by magnetized wind. The meridional circulation is then not maintained and the mixing of chemical elements is weaker. On the other hand, atomic diffusion is very efficient close to the surface so the thinner the surface convective zone, the more efficient the diffusion. The combination of the two effects leads to large surface abundance variations.
3.1.2. Impact of radiative acceleration
To quantify the effects of radiative acceleration, we now consider models A3, B3, B4, C3, and C4, which are identical to models A1, B1, B2, C1, and C2, respectively, except that they do not include radiative acceleration. We identify again three regimes:
– We find that the effect of radiative acceleration is negligible for the 1.3 M_{⊙} models (models A1 and A3 are similar) because their convective envelopes are too deep.
– For the 1.4 M_{⊙} model, we do not find any accumulation of iron due to radiative acceleration (but a moderate depredion) contrarily to what was obtained in Deal et al. (2018) for a 1.4 M_{⊙} model at solar metallicity, but with no rotationnaly induced mixing (see their Fig. 1). This shows that rotationally induced mixing is strong enough to prevent the accumulation due to radiative acceleration. Moreover, the comparison of models that include radiative acceleration (B2) with models that do not (B4) in Fig. 2 shows that radiative acceleration does not counteract rotational mixing, but mitigates the gravitational settling. As part of atomic diffusion, the radiative acceleration alone induces an iron surface abundance difference reaching from 0.05 dex for an initial rotation speed v_{ini} = 80 km s^{−1} to 0.1 dex for v_{ini} = 30 km s^{−1} (not shown in the figure).
Fig. 2. Evolution of the surface [Fe/H] in dex with ν_{max} for 1.4 M_{⊙} models (B2 and B4) and 1.44 M_{⊙} models (C2 and C4) with an initial rotation speed of 80 km s^{−1}. Models including atomic diffusion with (respectively without) radiative acceleration are shown with solid (respectively dashed) lines. 

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– At 1.44 M_{⊙}, we find different types of behaviour depending on whether radiative acceleration is taken into account: with radiative acceleration iron accumulates at the surface (model C2, Fig. 2), while without it iron is strongly depreded (model C4). The difference reaches ≈0.6 dex. With or without radiative acceleration, as the surface convective zone at 1.44 M_{⊙} is thin, atomic diffusion is efficient, while the extraction of angular momentum is not. With or without radiative acceleration, atomic diffusion leads to strong surface abundance variations, much greater than is expected from observations.
These results show how important it is to take into account all atomic diffusion processes in this range of mass ([1.4;1.44] M_{⊙}) for a more coherent and realistic physical description. The fact that its effects may be in contradiction with observations points towards some missing additional mechanism in the stellar modelling. Atomic diffusion (including radiative acceleration) is crucial when the impact of competing transport processes is weak.
The predicted large element depredion (at least for the studied elements) is not observed. The surface abundances of stars with thin surface convective zones show weak surface abundance depredion or accumulation. This indicates that there is a need for additional transport processes or a revised formulation of rotationally induced transport in order to reproduce the observations. This conclusion was already reached when studying the impact of atomic diffusion alone. The modelling of this type of star required the inclusion of an ad hoc turbulence (e.g. Richer et al. 2000; Richard et al. 2001; Michaud et al. 2011; Verma & Aguirre 2019) to be consistent with observations. This conclusion still holds when including rotationally induced mixing as implemented in CESTAM for these masses.
3.1.3. Atomic diffusion and magnetic braking
As discussed in Sect. 2.3, atomic diffusion and rotation are strongly coupled and this is mainly due to magnetic braking.
Impact of magnetic braking on mixing. The main process controlling the efficiency of the rotationally induced mixing is the extraction of angular momentum at the surface. Without it, the mixing would be rather weak. Figure 3 shows the profile of D_{turb, rota} for models B1 and B5. When there is a loss of angular momentum at the surface, the mixing is 1.5 orders of magnitude stronger at the bottom of the surface convective zone (solid curve). This implies a stronger reduction of the efficiency of atomic diffusion. When the extraction is negligible, atomic diffusion dominates. So the way we model the transport of angular momentum and its extraction is a key point for the transport of chemical elements.
Fig. 3. Turbulent diffusion coefficient induced by rotation (upper panel) and rotation profile (lower panel) as a function of log(ΔM/M^{*}) (ΔM is the mass above the considered region and M^{*} is the mass of the star) at 1 Gyr for 1.40 M_{⊙} models. The solid line corresponds to model B1 with magnetic braking, whereas the dashed line is for model B5 without magnetic braking. The surface of the star is on the left of the figure. 

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Impact of atomic diffusion on magnetic braking. The extraction of angular momentum through magnetized winds depends on the ability of the star to maintain a magnetic field thanks to the dynamo process. This mainly depends on the size of the convective envelope and on processes that may affect it. The thicker the envelope, the more efficient the braking of the star. In particular, the size of the convective zone can be affected by atomic diffusion when heavy elements are accumulated and induce a local increase in the opacity (e.g. Turcotte et al. 1998b; Deal et al. 2018). To illustrate this effect on opacity, we computed a model (C5), which is the same as C2, but in which we did not recompute the Rosseland mean opacity at each mesh point and each time step when the mixture is affected by diffusion. In this model, because of the accumulation of heavy elements at the surface (especially iron in this case) the increase in opacity at the bottom of the surface convective zone is strongly underestimated. This explains why the size of the surface convective zone is smaller in model C5 than in model C2, as shown in the top panel of Fig. 4. The maximum relative difference in the convective zone mass reaches 45%.
Fig. 4. Evolution of the mass of the surface convective zone (top panel) and of the surface rotation speed (middle panel) of the 1.44 M_{⊙} models (C2 and C5). In model C5, the opacities are calculated from an OP opacity table assuming a fixed solar mixture of chemical elements (dashed curves), while in model C2 the opacities are calculated for the actual composition with the OPCD package. Lower panel: D_{turb, rota} profile for both models at 1 Gyr. 

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As the convective zone is larger when accounting properly for the abundance variations and opacities, the braking due to magnetized wind is then more efficient. Figure 4 (middle panel) shows the evolution of the rotation speed with time. The rotation speed of the C2 model is slower than that for the C5 model. The difference reaches a maximum of 1 km s^{−1}. The enhanced efficiency of the extraction of angular momentum in model C2 leads to a mixing induced by the rotation that is 40% stronger than in model C5 (between log(ΔM/M^{*}) = − 6 and −4). As the mixing is less efficient in C5, the accumulation of iron in the surface convective zone is then greater.
This example is a good illustration of the coupling that exists between transport processes. In this case the coupling occurs through opacity, due to the variation of the chemical composition with time. This confirms that it is no longer possible to use opacity tables with a fixed mixture of chemical elements for this type of star when mixing processes affecting elements individually are taken into account. Computation of stellar models then requires opacity tables such as those provided by the publicly available OPCD package, for example.
3.2. Uniform versus differential rotation
The theory of the transport of angular momentum and associated transport of chemicals in stars is still far from being understood. The observations show that the current theory underestimates the transport of angular momentum between the core and the surface of stars, low and intermediate mass mainsequence stars tending to rotate nearly uniformly in their radiative regions (e.g. Deheuvels et al. 2012; Aerts et al. 2019; Ouazzani et al. 2019; Buldgen 2019).
Accordingly in this section, we study the impact on the surface abundances of a uniform rotation maintained along the mainsequence evolution. We build stellar models assuming solid body rotation under the assumption that the angular momentum transport is efficient enough to maintain a uniform rotation despite structural changes and hydrodynamical instabilities. We further assume that this extra transport of angular momentum does not affect the mixing of chemical elements. In this framework the modelling assumes neither shearinduced transport nor meridional circulation. The characteristics of the models (A6, B6, and C6) are listed in Table 2. We use a value of 8.3 × 10^{30} erg for the constant of the extraction of angular momentum in models with uniform rotation taking into account Matt et al. (2019) recommendations.
Inputs of the models with uniform rotation.
Figure 5 shows the surface abundances of iron, helium, and carbon for the 1.4 M_{⊙} models. As there is no transport of chemical elements induced by rotation, the only impact on the transport is due to the inflation of the star due to rotation. As a consequence, the effects of atomic diffusion are not reduced and the surface abundances of helium and carbon are not consistent with observations (e.g. Ghazaryan et al. 2018; Verma et al. 2019). The increase in the initial rotation speed helps to reduce the impact of atomic diffusion, but an initial speed of 80 km s^{−1} is still not sufficient (green curves in Fig. 5).
Fig. 5. Evolution of [Fe/H] in dex (top panel), helium Y_{Surf} in mass fraction (middle panel), and the surface [C/H] in dex (lower panel) as a function of ν_{max} for 1.4 M_{⊙} models with differential (solid curves) and uniform (dashed curves) rotation at two rotation speeds. Horizontal dotted lines represent the initial abundance. 

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We also investigated the case where a uniform rotation is induced by an unknown additional transport of angular momentum. We do so as in Eggenberger et al. (2019, and references therein) by including an additional viscosity, ν_{V, add} = 10^{8} cm^{2} s^{−1}, (i.e. D_{v} + ν_{V, add} in Eq. (2)). The value is calibrated by Ouazzani et al. (2019) on γDoradus stars. We assume that this additional transport of angular momentum does not impact directly the transport of chemical elements. In this case the shearinduced transport is negligible and the only transport of chemical elements comes from the interaction between meridional circulation and horizontal shear turbulence. This interaction results in a process that behaves like a diffusive process with a coefficient given by D_{eff} = (rU_{2})^{2}/30D_{h}. In our case the value of D_{h} is very high compared with (rU_{2})^{2}, and D_{eff} is therefore low. The transport of chemical elements is thus negligible. The resulting surface abundances are similar to the above case of imposing directly a uniform rotation.
From here on, we conclude that in the framework of a forced solid body rotation with no impact on rotational mixing, only chemically peculiar stars (Fm stars in the 1.4 M_{⊙} and 1.44 M_{⊙} cases) should exist and be observed. However, this scenario is not supported by observations of most of the Kepler stars (Bruntt et al. 2012; Brewer et al. 2016). This indicates that an extra transport process of chemical elements is also missing, likely associated with the extra angular momentum transport needed to account for observations.
4. Inferring stellar parameters from observational constraints
Our goal in this section is to estimate the impact of neglecting rotation and atomic diffusion in stellar models on the inference of stellar parameters. For this purpose, we compare the true stellar parameters of artificial stars with those obtained by the AIMS optimization code (Lund & Reese 2018; Rendle et al. 2019) using a grid of models in which these ingredients are lacking. The artificial stars are represented by the models previously discussed, (A1, A3, B1, B3, C1, C2, C3, C4) in which transport by rotation and diffusion are taken into account, the models of 1.3 and 1.4 M_{⊙} including radiative acceleration of Deal et al. (2018), and models of 1.3 and 1.4 M_{⊙} including the same physics as the grid for test purposes. We first describe the methodology.
4.1. AIMS optimization code
The AIMS optimization code applies a Markov chain Monte Carlo (MCMC) approach in order to find a representative sample of stellar models that fit a given set of classic and seismic constraints. This sample is subsequently used to find the bestfitting values, error bars, and posterior probability distribution functions (PDFs) for the different stellar properties. In order to gain computation time, the AIMS code uses a precomputed grid of stellar models which includes global stellar properties such as mass and age as well as pulsation spectra, and interpolates within this grid for each MCMC iteration. Interpolation is carried using a multidimensional Delaunay tessellation between evolutionary tracks and a simple linear interpolation along evolutionary tracks. For the seismic constraints, AIMS will treat the pulsation frequencies as independent normally distributed random variables. During the fitting process, it is possible to fit frequency combinations such as frequency ratios rather than individual frequencies; AIMS will automatically calculate the resultant correlation matrix for such combinations. For the classic constraints, a wider variety of probability distribution functions can be applied. In what follows, we used normal distributions, truncated at 1σ, in order to avoid having the optimization method go into the wings of the probability distribution.
4.2. Input to AIMS: Grids of stellar models and associated oscillation frequencies
When using the AIMS code, we consider grids of stellar models that do not include any transport processes but convection. The other input physics are kept the same as for the artificial stars (Table 1). The stellar models of the grids are also computed with the CESTAM code. The oscillation frequencies are computed using ADIPLS (ChristensenDalsgaard 2008) for l = [0, 3] and n = [0, 30]. The characteristics of grid 1 (hereafter the standard physics grid) are presented in Table 3.
Parameters of the grids used in the AIMS stellar parameter optimization pipeline.
4.3. Input to AIMS: the observational constraints of the artificial stars
We used the usual classical constraints (T_{eff}, luminosity, and [Fe/H]) and included for the seismic constraints the individual oscillation frequencies with degree l = 0–2. We computed the frequency at maximum power ν_{max} using a scaling relation (Kjeldsen & Bedding 1995) and chose ten frequencies above and below ν_{max}. The uncertainties on the frequencies were set to 0.5 μHz and for the classical constraints 70 K (T_{eff}), 0.05 (luminosity), and 0.1 dex ([Fe/H]).
We ended up with ≈63 individual frequencies and three classical parameters for the observational constraints. We also carried out inference optimization using frequency ratios rather than individual frequencies. In that case, we also added Δν_{moy} (the mean large frequency separation) and the three lowest frequencies of l = 0 to the set of constraints. The inclusion of low individual frequencies allows us to better constrain the mass (Serenelli, priv. comm.), while not being too sensitive to surface effects. The number of frequencies is quite large because our aim is to assess how large the systematic errors are on the stellar parameter determination when the physical description of chemicals transport is not properly modelled. We nevertheless also tested cases in which the l = 2 frequencies were removed, or the frequency uncertainties were reduced to 0.1 μHz. The results were identical.
4.4. Testing the accuracy of the AIMS code
The AIMS code is a powerful tool for inferring stellar parameters, but its precision depends on the stellar model grid it uses (Rendle et al. 2019). In order to determine the uncertainties using grid 1, as pseudotarget stars we chose models with the physics of grid 1, but that do not belong to the grid. The adopted models for the pseudotarget stars are listed in Table 4.
Parameters of the test models.
The comparison between the parameters of the input models and the determination with AIMS using grid 1 are presented in Table 5. We can see that a precision of the order of 2.9% is obtained for the mass, 7.5% for the age, and 1% for the radius when using individual frequencies. In most of these six cases, AIMS finds the exact value; the most uncertain parameter is the helium content. Adding the helium content as an observational constraint is definitely helpful in lifting the degeneracy (Mass/Y). For example, for the A8 model, the mass inference goes from 1.33 to 1.325 M_{⊙} (using grid 1) when helium is added as an observational constraint. The mass inference is 1.32 M_{⊙} when using grid 2 (denser grid, see Table 5), and goes to 1.29 M_{⊙} when taking into account the helium constraint.
Results of the optimization for the test models.
The differences in age, mass, and radius are shown in Fig. 6. This figure represents the departures of the values inferred by AIMS from the values of the input models. Uncertainties of 2σ, obtained from the AIMS probability distributions, were adopted for each parameter. We note that when the uncertainties appear unreasonably small, it only means that the number of accepted models in the grid is small, taking into account the observational constraints. This signals (except for model A8) that the physics of the grid is too different from the input models to find a reliable solution. This is mainly due to the [Fe/H] constraint, as the chemical composition is the main difference between the grid and inputs models. For model A8, by construction, the small uncertainties cannot come from a different physical description; they are due to a small number of accepted models. The results improve slightly when using grid 2. We conjecture that for this model, the problem comes from the density of the grid.
Fig. 6. Deviation between the real value of mass, age, and radius, and the inferred value by AIMS (using grid 1). Left panel: results for the 1.3 M_{⊙} model and right panel: results for the 1.4 M_{⊙} model. The crosses (blue: X_{c} = 0.6, red: X_{c} = 0.4, green, X_{c} = 0.2) represent the deviations with 2σ uncertainties from AIMS probability distributions. 

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We performed the same comparison using a second set of constraints (i.e. frequency ratios, mean Δν, and the three lowest l = 0 frequencies) instead of individual frequencies as seismic constraints. The precision is slightly worse than when using individual frequencies. Ratios appear less effective than individual frequencies. This must be attributed to the fact that in our theoretical study with individual frequencies, our set of frequencies is quite large with many low frequencies (best suited to constrain the structure). In such ideal cases (where no surface effects pollute the frequencies), the optimization using individual frequencies is quite efficient at finding an optimal model. Reducing by a factor of two the number of frequencies provided results with individual frequencies equivalent to those obtained with frequency ratios. We then decided to continue this study using only the large set of individual frequencies as seismic constraints.
The same tests were performed using grid 2 presented in Table 3. This grid covers the same mass range, but a narrower range of chemical compositions. It is finer and the time steps between models was divided by a factor of two. The maximum errors on age using individual frequencies and grid 1 was 7.5% for model D. With this grid the error drops to 1.6%. All the other determinations are slightly improved, with error reductions of a few 0.1%, but the worst cases are drastically improved. The error on the parameter determinations comes mainly from the quality of the grid, but the method is robust. Computing a new grid with the resolution of grid 2 but the range of parameters of grid 1 would have required too many computation resources and would not have changed the conclusion of this paper. This is the reason why we performed the study with grid 1.
4.5. Solar case
As a further test we consider the solar case. We studied on the one hand a model close to the solar model with parameters included in the grid, and on the other hand a set of noisy frequencies, taken from Silva Aguirre et al. (2017), which were determined from solar data but degraded to the level of quality corresponding to the Kepler observations. We computed a new grid that includes the same physics as grids 1 and 2, but takes into account atomic diffusion (without radiative acceleration). The properties of the grid are [0.9; 1.1; 0.025] M_{⊙} for the mass, [0.22; 0.27; 0.01] for Y_{ini}, [0.010; 0.018; 0.002] for Z_{ini}, and [0.6; 0.8; 0.02] for α_{CGM}. No core overshoot is taken into account. We use the twoterm surface correction expression from Ball & Gizon (2014) to account for surface effects in the real data.
The results obtained using AIMS (2σ errors) for the model are a mass of 0.997 ± 0.011 M_{⊙} (model mass: 1.0 M_{⊙}), a radius of 0.998 ± 0.007 R_{⊙} (model radius: 0.999 R_{⊙}), and an age of 4.672 ± 0.400 Gyr (model age: 4.606 Gyr). The degraded solar data gave us a mass of 0.987 ± 0.014 M_{⊙}, a radius of 0.994 ± 0.042 R_{⊙}, and an age of 4.845 ± 0.140 Gyr. In both cases the method and the grid give results very close to the real values of the Sun’s parameters.
5. Impact of neglecting transport processes on stellar parameter inference
In this section we assess the impact of neglecting atomic diffusion (including radiative acceleration) and/or rotationally induced mixing on the seismic inference of stellar parameters (mass, radius, age, chemical composition).
5.1. Models with atomic diffusion and without rotation
We first tested the impact of atomic diffusion (including radiative acceleration) on the stellar parameter determinations. To this end, we used the 1.3 and 1.4 M_{⊙} models at solar metallicity presented in Deal et al. (2018) at three epochs on the main sequence. These models include atomic diffusion unlike our stellar model grid. They do not include rotationally induced mixing. The results from the optimization are presented Fig. 6. The same trend with evolution seems to appear for 1.3 and 1.4 M_{⊙} models. The deviation from the true age increases up to X_{c} = 0.4 and then decreases at X_{c} = 0.2 (or at least is not larger for the 1.4 M_{⊙} model). This deviation is caused by a difference in the surface iron content, [Fe/H]. Since we considered a grid without transport of chemical elements in the radiative regions the models of the grid therefore keep the same [Fe/H] all over the main sequence. This is not the case for the models representing the artificial stars for which we want to determine the stellar parameters because they include atomic diffusion. In order to match the value of the [Fe/H] of the artificial star at its evolutionary stage, the optimization method then searches for a model with a different [Fe/H] than the value at birth. The optimization process will infer an incorrect set of stellar parameters, mainly a wrong age, due to this metallicity effect. The deviation is smaller at the end of the main sequence because the surface convective zone starts deepening and erasing the abundance variations created during the evolution. The impact on the age is larger when the observed models have a surface [Fe/H] lower than the initial value (1.3 M_{⊙} models, low effect of radiative acceleration on iron) rather than the opposite (1.4 M_{⊙} models, large effect of radiative acceleration on iron).
The deviations for the radius and for the mass at X_{c} = 0.6 and 0.4 are very small and they increase at the end of the main sequence. As the star evolves, atomic diffusion has more time to act. One of the effects of radiative acceleration, in particular, is to reduce the density in the affected regions. This causes a more significant increase in the radius at the end of the main sequence. For a given Δν (i.e. a given mean density), a larger radius translates directly into a higher inferred mass.
The deviations are most of the time below 5% and 2% for the mass and radius, respectively, but the age is strongly impacted (above 10%). These results are upper limit deviations because atomic diffusion is in competition with other transport processes. It is important to keep in mind that this process occurs in any case, and can lead to significant errors in parameter inference when neglected.
5.2. Models with rotation and atomic diffusion
We now turn to the case where some competition exists between atomic diffusion and rotationally induced mixing.
5.2.1. Without radiative acceleration
We first tested the impact of taking rotation and diffusion without radiative acceleration into account in the models on stellar parameter inference (models A3, B3, C3, and C4 of Table 1). The initial rotation speed is 30 km s^{−1} for the 1.3 and 1.4 M_{⊙} models, and both 30 and 80 km s^{−1} for the 1.44 M_{⊙} models. The deviation of AIMS inferences from the real values are presented Fig. 6.
For the 1.3 M_{⊙} models, the age deviation remains small over the entire main sequence. The important mixing induced by rotation limits the variations of the surface [Fe/H] due to atomic diffusion, which therefore remains small. At a given evolutionary state, rotation induces an effective gravity which is weaker than that of an equivalent star without rotation. At a constant mass, it induces a larger radius. At a given mean Δν the optimization will then infer a higher mass.
For the 1.4 M_{⊙} models, the impact of atomic diffusion has become strong, while the efficiency of the extraction of angular momentum has decreased enough so that the surface abundances significantly vary compared with their initial values. This leads to inferred age values which significantly deviate from the real value. The maximum deviation occurs for X_{c} = 0.4 when the [Fe/H] is more than 0.1 dex lower than the initial value. The deviation of the radius is smaller than for the 1.3 M_{⊙} models, hence leading to a smaller deviation in mass.
The 1.44 M_{⊙} models (Fig. 7) show even larger age deviations than the 1.4 M_{⊙} models due to larger [Fe/H] variations during the main sequence; however, the radii and masses are quite well recovered by AIMS despite the use of the standard physics grid. The impact of the initial rotation speed is mainly visible on the radius deviations, which increase with the rotation speed.
Fig. 7. Deviation between the real value of mass, age, and radius, and the inferred value by AIMS (using grid 1) for 1.44 M_{⊙} models. The legend is the same as Fig. 6. 

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In a nutshell, the main impact of rotation or diffusion on the stellar parameter inference is upon the age, as expected. The impact on the age can be larger than 1 Gyr for stars with masses higher than 1.4 M_{⊙} models. These examples show that for stars with masses higher than 1.3 M_{⊙} both processes should be taken into account, which allows more accurate stellar parameters to be inferred.
5.2.2. With radiative acceleration
When inference of stellar parameters is carried out for models including radiative acceleration (i.e. models A1, B1, C1, and C2), the impact is smaller than when including rotation. For the 1.3 M_{⊙} models, the inferences are almost identical because the radiative acceleration is not efficient (Fig. 6). In the other cases (1.4 and 1.44 M_{⊙} models) the scatter around the real values of age, mass, and radius are smaller than that due to rotation (see Figs. 6 and 7).
For the 1.4 M_{⊙} models, the maximum difference in age is 0.6 Gyr and goes down to 0.35 Gyr when radiative acceleration is taken into account. At 1.4 M_{⊙} it goes from 0.8 to 0.2 and from 1.15 to 0.3 Gyr for models with a surface initial rotation speed of 30 and 80 km s^{−1}, respectively. This occurs because radiative acceleration reduces the [Fe/H] variations and makes [Fe/H] closer to its initial value. The deviation from the standard models then remains small. For the mass and radius, the reduction of the deviation is smaller in both the 1.4 and 1.44 M_{⊙} models.
As already mentioned, the transport of angular momentum is underestimated in the current rotating models (e.g. Deheuvels et al. 2012; Aerts et al. 2019; Ouazzani et al. 2019; Buldgen 2019). When considering uniformly rotating models equivalent to those presented in Sect. 3.2, atomic diffusion dominates over the mixing induced by rotation and the impact on the age is more significant (close to the deviations presented in Sect. 5.1). Hence, like the transport of chemical elements, the transport of angular momentum is a key to building models with accurate stellar parameters for solarlike oscillating stars.
5.3. Impact of core overshoot on the age
The uncertainties on ages due to rotation and atomic diffusion can also be compared with those arising from uncertainties on the core overshoot extension. We computed models with the same input physics as model A1, but without rotation. We computed the opacities with the OP opacity table instead of the OPCD package, and tested that it has no impact on the age at the end of the main sequence. We assumed several values for the extension of the core overshoot. We determined that in order to obtain the same age at the end of the main sequence as in model A1, using a model that does not take rotation into account, the core overshoot should be 0.18 H_{p} (instead of 0.15 H_{p}). The age difference at the end of the main sequence between model A1 and the same model without rotation is 120 Myr (≈3% of the total age). A slight degeneracy appears here between the impact on the age of rotation and core overshoot.
5.4. Kepler Legacy stars
Kepler Legacy stars KIC 2837475, KIC 9206432, KIC 11081729, and KIC 11253226 are stars potentially affected by inaccuracies in the stellar parameter inferences due to an improper modelling of transport processes in their radiative interiors. The stellar parameters for the four stars are listed in Table 6. All four stars have inferred masses between 1.32 and 1.46 M_{⊙} with metallicities around the solar value. Their surface rotation velocities are less than 25 km s^{−1} and the range of ν_{max} is in the region where abundance variations are predicted to be the most important (see Figs. 1 and 5). This implies that the currently determined stellar parameters are possibly overestimated by [0.05,0.08] M_{⊙} (≈3 − 5%) for the mass, 0.4 Gyr (≈25%) for the age, and 0.04 R_{⊙} (≈2.5%) for the radius. Age and radius errors due to neglecting atomic diffusion (with radiative acceleration) and rotation are similar to the dispersion obtained by Silva Aguirre et al. (2017), but the error on the age is much larger (except for KIC 9206432, which is around 20%). Inferring the parameters of these stars with a grid of models including atomic diffusion (with radiative acceleration) and rotation would then lead to significantly different ages. This of course strongly depends on the metallicity because the transport of chemical elements by atomic diffusion and rotation depends on the size of the surface convective zone. At a given mass, the size of the surface convective zone is not the same depending on the metallicity. The effect is then most likely greater when the metallicity is lower at a given mass (i.e. higher for KIC 11253226 than KIC 9206432). A specific modelling of these four stars taking into account atomic diffusion and rotation will be performed in a forthcoming paper, as will the individual modelling of stars in the three predicted regimes.
Parameters of the Kepler Legacy targets from Lund et al. (2017) and Silva Aguirre et al. (2017).
Another possibility to infer the parameters of these stars would be to use local optimization methods such as those based on the Levenberg–Marquardt minimization (Miglio & Montalbán 2005; Lebreton & Goupil 2014). These methods have the advantage that they allow us to easily explore wider ranges of possible input physics and parameters on the fly, and they do not require us to calculate a grid of models for each of them. However, they require some care, due to risks related to possible local minima, and they cost more in computational time. They will be investigated in a forthcoming paper.
5.5. Impact of the mixinglength parameter
For all the models considered in this work, we chose to keep the same α_{CGM}. This choice was made in order to be able to compare the models with exactly the same physics except for the processes we wanted to test (atomic diffusion, rotation) and to study their intrinsic impact.
In order to estimate the impact of keeping the same value for the mixinglength parameter, we computed a model of 1.4 M_{⊙} (the same as A8) with a solar calibrated α_{CGM} = 0.633 (instead of α_{CGM} = 0.68) and solar calibrated initial chemical composition. Then we inferred the parameters of this model using grid 1. We found a mass 0.06 M_{⊙} lower, a radius 0.02 R_{⊙} smaller, and an age 0.2 Gyr older. This means that by not using the solar calibrated α_{CGM} value and the initial chemical composition, we probably underestimate masses and radii and overestimate ages. In almost all the cases presented in Sect. 5, we found that neglecting atomic diffusion (including radiative acceleration) and rotation leads to an overestimation of masses, radius, and ages when using grid 1. The net effect when using solar calibrated values in accordance with the physical assumptions is expected to be an even larger overestimate of the mass and a smaller one for the age when neglecting diffusion and rotation. We note, however, that even in this case our predicted impact on the age is larger than that coming from the different mixinglength parameter values.
We also note that there is no reason a priori to use the solar calibrated values for stars more massive than the Sun. The mixinglength parameter was indeed found to vary with evolution and mass (e.g. Freytag et al. 1999; Trampedach et al. 2014; Sonoi et al. 2019). Sonoi et al. (2019) showed that the α_{CGM} value can vary from 0.583 to 0.801 for stars with T_{eff} = [4018;6725] K and log g = [1.50;4.50] dex, while the calibrated solar value was 0.69. For example, their computations of the mixinglength parameter for a model close to our A8 model gives α_{CGM} = 0.636 (see their Table A.1).
To minimize this source of uncertainties, we plan to build a grid of models including atomic diffusion (including radiative acceleration) and rotation, and taking into account various values of α_{CGM} and the overshoot parameter as well.
6. Conclusion
We studied the impact of taking both atomic diffusion and rotationally induced mixing into account on surface abundances and inferences of stellar parameters such as mass, age, and radius for mainsequence stars with masses in the range [1.3–1.44] M_{⊙}. Atomic diffusion here includes radiative acceleration, and rotation is assumed to be either differential in radius or uniform. We showed that a strong interaction between atomic diffusion and rotation exists throughout the size of the convective envelope. The accumulation of elements at the surface leads to an increase in the surface convective zone due to a local increase in the opacity. As the surface convective zone is larger, it is able to maintain a stronger magnetic field by dynamo. This generates a more efficient extraction of angular momentum by magnetized wind, and a stronger mixing induced by rotation, which in turn tends to decrease the effect of atomic diffusion.
We showed that the efficiency of the transport of chemical elements is strongly related to the efficiency of the transport of angular momentum. Atomic diffusion and rotation are then in competition. We considered a grid of standard stellar models; here standard means convection but no transport in radiative regions. A comparison of these models with models including rotationally induced mixing and/or atomic diffusion led us to distinguish three regimes depending on the mass of the star.
For stars with masses below and close to 1.3 M_{⊙}, when only atomic diffusion is taken into account, the inferred ages depart significantly from the actual ones. This is mainly due to the surface [Fe/H], which differs from the initial one (up to 0.15 dex). This large difference in age almost totally vanishes when shellular rotation is also taken into account. The mixing induced by the rotation indeed prevents large variations of surface abundances (helium and metals). The surface abundances are then consistent with observations. The efficiency of the rotationally induced mixing is due to an efficient extraction of angular momentum by magnetized wind, possibly because the size (atomic diffusioninduced, and so larger) of the surface convective zone is sufficient to maintain a magnetic field. In this mass range, when rotation is taken into account, radiative acceleration has a very small effect on surface abundances. The deviation in mass and radius comes from the effect of rotation on the structure of the star. We must note that the behaviour of surface abundances in this mass range is expected to be strongly affected by additional angular momentum transport processes (e.g. internal gravity waves).
For stars with masses close to 1.4 M_{⊙}, when only atomic diffusion is taken into account, the effect on the inferred age is the same as in the 1.3 M_{⊙} case. As the surface convection is thinner, the extraction of angular momentum by magnetized wind is less efficient. The mixing efficiency of rotation is weaker. Hence, when both atomic diffusion and rotation are considered, surface abundance variations are maintained, unlike for the lower mass case. The [Fe/H] variation reaches 0.1 dex, and helium is depreded down to ≈0.20, which is still consistent with observations. As [Fe/H] is lower than the initial value during the evolution on the main sequence, the age inference deviates from the real value by as much as 0.4 Gyr when using a standard physics grid. This is roughly 20–25% of the age when considering Kepler stars (see Sect. 5.4). In this mass range, radiative accelerations are crucial and have a significant effect on surface abundances (0.1 dex) and on stellar parameter inference.
For stars with masses higher than 1.4 M_{⊙}, surface abundance variations are quite large with or without rotation. Iron is accumulated at the surface due to radiative acceleration. Without rotation it is not possible to find a solution using a standard grid of stellar models. When the effect of rotation is included, inference of stellar parameters using a standard physics grid leads to important age deviations compared with the real value due to these large [Fe/H] differences. Radiative acceleration is crucial for parameter inference as rotation is no longer able to prevent the strong surface abundance depredion or accumulation. Surface abundances are no longer representative of normal Ftype stars, but are representative of Fm chemically peculiar stars in the range of initial surface rotation speeds (< 100 km s^{−1}) we considered. This is in disagreement with the surface abundance determinations of Kepler stars. We must then conclude that there is a missing transport process of chemical elements in addition to those of atomic diffusion and rotationally induced mixing as currently modelled.
All the comparisons presented in this study were done at constant X_{C}. It is known that some effects may be compensated when comparing at constant ν_{max} for instance. The results may differ slightly when performing a full optimization with a stellar model grid including atomic diffusion and rotation. The next step of the study is to perform these optimizations. We also plan to compare the results given by another optimization method (based on the Levenberg–Marquardt algorithm) in order to test the robustness of our conclusions. It will also allow us to test the impact of using a local method instead of a global one, AIMS for instance. We note that the above conclusions are based on stellar models with solar metallicity. For lower metallicities, the mass thresholds are smaller.
We also note that in most of the present study shellular rotation was assumed. However, observations show that the actual transport of angular momentum implemented in evolutionary codes is underestimated. Nowadays a consensus seems to hold where stars are likely rotating uniformly rather than differentially radially in their radiative regions. We therefore also considered a uniform rotation, which led to a small transport of chemical elements, hence to a stronger impact of atomic diffusion as early as 1.3 M_{⊙}. In that case, unlike shellular rotation, metal and helium levels are not compatible with observation. The missing transport processes of angular momentum and of chemical elements are potentially related. Despite the current uncertainties about the modelling of angular momentum transport, which also have consequences on the transport of chemical elements, the three regimes should exist even if the modelling of these processes is improved. The main impact will be the mass range for which each regime occurs.
One signature of transport of chemical elements in stars is the surface abundance of lithium. It traces the mixing occurring from the surface down to the region where lithium is destroyed by nuclear reactions (T = 2.5 × 10^{6} K). The lithium abundances of stellar models including rotationally induced mixing with shellular rotation are consistent with the hotter part of the lithium dip, as already emphasized long ago (e.g. Talon 2008). A more detailed study of the impact of the coupling between atomic diffusion (with radiative acceleration) and rotation on lithium is postponed to a forthcoming paper.
Acknowledgments
We thank Aldo Serenelli for fruitful discussions. We thank the referee Patrick Eggenberger for valuable comments which helped to improve the paper. This work was supported by FCT/MCTES through national funds (PIDDAC) by this grant UID/FIS/04434/2019 and by FEDER – Fundo Europeu de Desenvolvimento Regional through COMPETE2020 – Programa Operacional Competitividade e Internacionalização by these grants: UID/FIS/04434/2019; PTDC/FISAST/30389/2017 & POCI010145FEDER030389. MD is supported in the form of a work contract funded by national funds through Fundação para a Ciência e Tecnologia (FCT). This work was also supported by the CNES. We acknowledge financial support from the “Programme National de Physique Stellaire” (PNPS) of the CNRS/INSU cofunded by the CEA and the CNES, France.
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All Tables
Parameters of the grids used in the AIMS stellar parameter optimization pipeline.
Parameters of the Kepler Legacy targets from Lund et al. (2017) and Silva Aguirre et al. (2017).
All Figures
Fig. 1. Evolution of the surface [Fe/H] in dex (top panel), helium Y_{Surf} in mass fraction (middle panel), and the surface [C/H] in dex (lower panel) as a function of ν_{max} for different masses and initial rotation speeds for models including atomic diffusion with radiative acceleration. Horizontal dotted lines represent the initial abundance. The models are A1, B1, B2, C1, and C2 from Table 1. 

Open with DEXTER  
In the text 
Fig. 2. Evolution of the surface [Fe/H] in dex with ν_{max} for 1.4 M_{⊙} models (B2 and B4) and 1.44 M_{⊙} models (C2 and C4) with an initial rotation speed of 80 km s^{−1}. Models including atomic diffusion with (respectively without) radiative acceleration are shown with solid (respectively dashed) lines. 

Open with DEXTER  
In the text 
Fig. 3. Turbulent diffusion coefficient induced by rotation (upper panel) and rotation profile (lower panel) as a function of log(ΔM/M^{*}) (ΔM is the mass above the considered region and M^{*} is the mass of the star) at 1 Gyr for 1.40 M_{⊙} models. The solid line corresponds to model B1 with magnetic braking, whereas the dashed line is for model B5 without magnetic braking. The surface of the star is on the left of the figure. 

Open with DEXTER  
In the text 
Fig. 4. Evolution of the mass of the surface convective zone (top panel) and of the surface rotation speed (middle panel) of the 1.44 M_{⊙} models (C2 and C5). In model C5, the opacities are calculated from an OP opacity table assuming a fixed solar mixture of chemical elements (dashed curves), while in model C2 the opacities are calculated for the actual composition with the OPCD package. Lower panel: D_{turb, rota} profile for both models at 1 Gyr. 

Open with DEXTER  
In the text 
Fig. 5. Evolution of [Fe/H] in dex (top panel), helium Y_{Surf} in mass fraction (middle panel), and the surface [C/H] in dex (lower panel) as a function of ν_{max} for 1.4 M_{⊙} models with differential (solid curves) and uniform (dashed curves) rotation at two rotation speeds. Horizontal dotted lines represent the initial abundance. 

Open with DEXTER  
In the text 
Fig. 6. Deviation between the real value of mass, age, and radius, and the inferred value by AIMS (using grid 1). Left panel: results for the 1.3 M_{⊙} model and right panel: results for the 1.4 M_{⊙} model. The crosses (blue: X_{c} = 0.6, red: X_{c} = 0.4, green, X_{c} = 0.2) represent the deviations with 2σ uncertainties from AIMS probability distributions. 

Open with DEXTER  
In the text 
Fig. 7. Deviation between the real value of mass, age, and radius, and the inferred value by AIMS (using grid 1) for 1.44 M_{⊙} models. The legend is the same as Fig. 6. 

Open with DEXTER  
In the text 
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