# Signature of solar g modes in first-order p-mode frequency shifts

## TL;DR

This study evaluates how solar gravity (g) modes influence p-mode frequencies, finding the effects are extremely small and unlikely to be detectable through frequency shifts alone, thus challenging previous detection claims.

## Contribution

The paper provides the first quantitative analysis of first-order p-mode frequency perturbations caused by g modes, clarifying their minimal impact and the difficulty of detection.

## Key findings

- G modes perturb p-mode frequencies only if even harmonic degree and zero azimuthal order.
- Frequency shifts caused by g modes are smaller than 0.1 nHz, or 2×10⁻⁸ in relative terms.
- Structural changes dominate over advection in the interaction between g and p modes.

## Abstract

Context. Solar gravity modes (g modes) are buoyancy waves trapped in the solar radiative zone that have been very difficult to detect at the surface. Solar g modes would complement solar pressure modes (p modes) in probing the central regions of the Sun, for example the core rotation rate. Aims. A detection of g modes using changes in the large frequency separation of p modes has recently been reported. However, it is unclear how p and g modes interact. The aim of this study is to evaluate to what extent g modes can perturb the frequencies of p modes. Methods. We computed the first-order perturbation to global p-mode frequencies due to a flow field and perturbations to solar structure caused by a g mode. We focused on long-period g modes and assumed that the g-mode perturbations are constant in time. The surface amplitude of g modes is assumed to be $1$ mm s$^{-1}$, which is close to the observational limit. Results. Gravity modes do perturb p-mode frequencies to first order if the harmonic degree of the g mode is even and if its azimuthal order is zero. The effect is extremely small. For dipole and quadrupole p modes, all frequency shifts are smaller than $0.1$ nHz, or $2\times10^{-8}$ in relative numbers. This is because the relative perturbation to solar structure quantities caused by a g mode of realistic amplitude is of the order of $10^{-6}$ to $10^{-5}$. We find that structural changes dominate over advection. Surprisingly, the interaction of g and p modes takes place to a large part near the surface, where p modes spend most of their propagation times and g modes generate the largest relative changes to solar structure. Conclusions. It appears to be impossible to detect g modes solely through their signature in p-mode frequency shifts. Whether g modes leave a detectable signature in p-mode travel times under a given observational setup remains an open question.