Standard solar models in the light of new helioseismic constraints. II. Mixing below the convective zone

Citation
As. Brun et al., Standard solar models in the light of new helioseismic constraints. II. Mixing below the convective zone, ASTROPHYS J, 525(2), 1999, pp. 1032-1041
Citations number
72
Categorie Soggetti
Space Sciences
Journal title
ASTROPHYSICAL JOURNAL
ISSN journal
0004637X → ACNP
Volume
525
Issue
2
Year of publication
1999
Part
1
Pages
1032 - 1041
Database
ISI
SICI code
0004-637X(19991110)525:2<1032:SSMITL>2.0.ZU;2-H
Abstract
In previous work, we have shown that recent updated standard solar models c annot reproduce the radial profile of the sound speed at the base of the co nvective zone and fail to predict the photospheric lithium abundance. In pa rallel, helioseismology has shown that the transition from differential rot ation in the convective zone to almost uniform rotation in the radiative so lar interior occurs in a shallow layer called the tachocline. This layer is presumably the seat of a large-scale circulation and of turbulent motions. Here we introduce a macroscopic transport term in the structure equations that is based on a hydrodynamical description of the tachocline proposed by Spiegel & Zahn, and we calculate the mixing induced within this layer. We discuss the influence of different parameters that represent the tachocline thickness, the Brunt-Vaisala frequency at the base of the convective zone, and the time dependence of this mixing process along the Sun's evolution. We show that the introduction of such a process inhibits the microscopic di ffusion by about 25%. Starting from models including a pre-main-sequence ev olution, we obtain (1) a good agreement with observed photospheric chemical abundance of light elements such as He-3, He-4, Li-7, and Be-9; (2) a smoo th composition gradient at the base of the convective zone; and (3) a signi ficant improvement of the sound-speed square difference between the seismic Sun and the models in this transition region when we allow the photospheri c heavy-element abundance to adjust, within the observational incertitude, as a result of the action of this mixing process. The impact on neutrino pr edictions is also discussed.