The energy of waves in the photosphere and lower chromosphere: 1. Velocity statistics

TL;DR

This study investigates the energy carried by acoustic waves in the solar chromosphere using Ca II H spectral data, finding that wave energy alone is insufficient for chromospheric heating as modeled.

Contribution

It provides a detailed analysis of wave velocity statistics and energy flux in the chromosphere, comparing observations with semi-empirical models to assess wave heating.

Findings

Wave velocity amplitudes grow with height as predicted by linear theory.

Wave energy flux above 500 km height is insufficient for chromospheric heating.

Chromospheric intensity variations are driven by waves originating in the photosphere.

Abstract

Acoustic waves are one of the primary suspects besides magnetic fields for the chromospheric heating process to temperatures above radiative equilibrium (RE). We derived the mechanical wave energy as seen in line-core velocities to obtain a measure of mechanical energy flux with height for a comparison with the energy requirements in a semi-empirical atmosphere model. We analyzed a 1-hour time series and a large-area map of Ca II H spectra on the traces of propagating waves. We analyzed the velocity statistics of several spectral lines in the wing of Ca II H, and the line-core velocity of Ca II H. We converted the velocity amplitudes into volume and mass energy densities. For comparison, we used the increase of internal energy necessary to lift a RE atmosphere to the HSRA temperature stratification. We find that the velocity amplitude grows in agreement with linear wave theory and thus slower with height than predicted from energy conservation. The mechanical energy of the waves above around z~500 km is insufficient to maintain the chromospheric temperature rise in the semi-empirical HSRA model. The intensity variations of the Ca line core (z~1000 km) can be traced back to the velocity variations of the lowermost forming spectral line considered (z~ 250 km). The chromospheric intensity, and hence, (radiation) temperature variations are seen to be induced by passing waves originating in the photosphere.