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What curves ฮ”๐œˆ?

Hekker, Saskia

Abstract

What curves ฮ”๐œˆ? S. Hekker, Y. Elsworth, S. Basu, F. Ahlborn, L. Buchele, F. Espinoza-Rojas Stars are to first order described as spheres of gas. They do however deviate somewhat from homogenous spheres of ideal gas and these deviations are imprinted in their normal oscillation modes. One of these imprinted features is that the large frequency separation, ฮ”๐œˆ, in solar-like oscillators is not constant: it is curved as a function of frequency. Two questions arise naturally 1) what in the structure of the star is responsible for this second order variation of ฮ”๐œˆ, and 2) how does the variation depend on global properties of the star like mass and age. We analyse a few thousand red-giant stars to derive empirical relations between ๐›ผ (the curvature coefficient) and ฮ”๐œˆ. Comparing these empirical relations with those obtained from stellar evolution models shows that a) the ๐›ผ - ฮ”๐œˆ relation for red-giant branch stars is mass dependent, and b) that the ๐›ผ - ฮ”๐œˆ relations obtained from the models differ from the empirical ones. We also calculate sensitivity kernels for ๐›ผ that allow us to determine the regions responsible for the curvature.This will provide important insights for improving the physics in our models and reconciling the difference between the empirical ๐›ผ - ฮ”๐œˆ relationships and those based on models.

Full text

Under the assumption that the curvature is part of a damped sinusoid induced by a glitch, i.e. a change in the stellar structure on spatial scales smaller than the local wavelength of the oscillations, we find: with ๐ด the amplitude and ๐œ the acoustic radius of the glitch. ๐œ€๐‘ mod 1 ๐›ผ = curvature of acoustic low degree (โ„“) modes The sensitivity of the curvature across the star peaks where the first adiabatic exponent ฮ“1is reduced due to the He I and H I ionisation zones. ๐›ผ= ๐ด 4๐œ‹๐œ 2ฮ”๐œˆ ฮ”๐œˆ ๐‘›๐‘= ๐‘› + 1 ๐‘›๐‘= ๐‘› + 2 ๐‘›๐‘= ๐‘› + 3 ๐‘›๐‘= ๐‘› = ๐‘›๐‘ ๐‘›๐‘= ๐‘› โˆ’ 1 ๐‘›๐‘= ๐‘› โˆ’ 2 oscillation spectrum of a red-giant star S. Hekker (1,2), Y. Elsworth (3), S. Basu (4), F. Ahlborn(2), E. P. Bellinger(4), L. Buchele(1,2), F. Espinoza-Rojas(1,2) 1. Heidelberg University, 2.Heidelberg Institute for Theoretical Studies (HITS), 3. University of Birmingham, 4. Yale University Curvature of large frequency separation ๐œˆ๐‘›๐‘,โ„“=0 =ฮ”๐œˆ โˆ™๐‘›๐‘+๐œ€๐‘+เต— ๐›ผ2๐‘›๐‘โˆ’๐‘›๐‘ 2 frequency radial order large frequency separation offset central radial order ๐›ผ He I + H I ionisation