scieee AI-readable full text Open interactive document viewer

No intermediate coupling prescription needed on the red-giant branch

van Lier, Tobias; Müller, Jonas; Hekker, Saskia

Abstract

Red-giant stars resonate in two cavities - pressure modes can oscillate in the envelope, while the core allows for the propagation of gravity modes. Since the eigenfrequencies of these modes fall in a similar range, mixed modes form via coupling of the cavities across the intermediate evanescent zone (EZ). The asymptotic frequency pattern of mixed modes is governed by the coupling strength q. So far, the link of q to stellar structure has been derived for an explicitly narrow or wide EZ (i.e. strong or weak coupling, respectively). We aim to test the validity of both approximations during the evolution along the red-giant branch (RGB). To do so, we derived q from numerically calculated oscillation frequencies for a set of stellar models and compared the resulting values to those obtained from the strong and weak coupling approximation. We confirm that the EZ widens along the RGB, such that first the strong and later the weak coupling approximation is valid. Additionally, we find that the weak coupling approximation is serendipitously applicable in narrower EZs than expected. On the RGB, this allows to always estimate values for the coupling strength in one of the two well-known limits without a need for an intermediate prescription.

Full text

T. van Lier1,2, J. Müller1,2, S. Hekker1,2 1 Heidelberg Institute for Theoretical Studies, Schloss-Wolfsbrunnenweg 35, D-69118 Heidelberg, Germany 2 Zentrum für Astronomie Heidelberg (ZAH/LSW), Heidelberg University, Königstuhl 12, D-69117 Heidelberg, Germany [email protected] References: Hekker, S., Elsworth, Y., & Angelou, G.C. 2018, A&A, 610, A80 Paxton, B., Smolec, R., Schwab, J., et al. 2019, ApJS, 243, 10 Shibahashi, H. 1979, PASJ, 31, 87 Takata, M. 2016, PASJ, 68, 109 Townsend, R.H.D., & Teitler, S.A. 2013, MNRAS, 435, 3406–3418 Accepted by A&A: van Lier et al. 2025, Weak or strong: Coupling of mixed oscillation modes on the red giant branch 𝑞w𝜈max tends to underestimate in its applicability regime! coupling strength 𝑞 applicable applicable usable weak coupling 𝜈max in µHz evolution 𝑞w too high on early RGB 𝑞s too low on late RGB 𝑞s not meaningful when Brunt-Väisälä spike in EZ strong coupling Mixed modes oscillate as g-modes in the buoyancy cavity (core), as p-modes in the sound cavity (envelope), and decay in the EZ. Their eigenfrequency is offset from that of pure g-/p-modes. This offset is governed by the level of interaction (coupling) between the two cavities and parametrized by the coupling strength 𝑞. buoyancy cavity sound cavity log(fractional radius) “narrow” EZ: strong coupling 𝑞s (Takata 2016a) “wide” EZ: weak coupling 𝑞w (Shibahashi 1979) mixed mode eigenfrequency pattern (Townsend+ 2013) Brunt-Väisälä-frequency, Lamb-frequency (Paxton+ 2019) (cf. Hekker+ 2018) cavity properties & coupling 𝑞as via asymptotic fit g-mode p-mode mixed mode log(frequency) We tested which theoretical value 𝑞s/w (relating 𝑞 to the stellar structure in the EZ) is suitable to reproduce the value 𝑞as (observable in the pattern of mixed-mode frequencies) at different stages on the RGB, where the EZ has different widths. To do so, we compared all three values for a set of stellar models. EZ radiative (early RGB): 𝑞s applicable EZ convective (late RGB): 𝑞w applicable Intermediate regime: 𝑞w usable ⇒ no intermediate prescription needed! Cutoff EZ-width: 0.4 × local decay length Caveat: “Usability” is mass-dependent (okay for 1M⊙≤ 𝑀 ≤ 2M⊙) NEW!